source("../config/Rmarkdown_config.R") # 依赖包的导入和一系列 Rmarkdown 设置

Data Processing

数据精度问题

EK2002 作者使用的编程软件是 GAUSS,其数据文件大都是二进制的,无法用文本编辑器打开,只能用 GAUSS 打印到屏幕上,然后手动复制粘贴到文本文件中,以获得本项目的数据源。

然而,图形化界面的 GAUSS IDE,只能显示小数点后三位,这意味着手动复制粘贴的数据从一开始就是不精确的,会影响所有结果的精度。

只有在命令行风格的 GAUSS Terminal Interface 中打印,才能显示数据的完整位数。从这里复制粘贴,才能保证本项目中数据的精确度。

Read Data

# 一些标量常数
scalar <- jsonlite::fromJSON("../data/scalar.json")

# 国家代码表
country_table <- fread("../data/country_code.csv")

# 用于参数估计的数据,数值型变量大多经过了对数标准化
regression_data <- fread("../data/regression_data.csv")

# 19国50产业价格数据
price_table <- fread("../data/price.csv")

看一下数据结构:

country_table %>% prettify()
id code name
1 AL Australia
2 AU Austria
3 BE Belgium
4 CA Canada
5 DK Denmark
6 FI Finland
7 FR France
8 GE Germany
9 GR Greece
10 IT Italy
11 JP Japan
12 NE Netherlands
13 NZ New Zealand
14 NO Norway
15 PO Portugal
16 SP Spain
17 SW Sweden
18 UK United Kingdom
19 US United States
regression_data
price_table

Data Transforming

## scalar.json

N <- scalar$N # 国家数量
beta <- scalar$beta # 各国平均 beta
theta_estimates <- scalar$theta # 三种不同水平的theta值
## regression_data.csv

# 进出口国 index
c(import_country, export_country) %<-% regression_data[, c(1, 2)]


# 对数标准化的制造业双边贸易数据 ln(Xni/Xnn)
trade <- regression_data[, 4] %>% pull()

# ln(X'ni/X'nn), (26)式等号的左边
trade_prime <- regression_data[, 5] %>% pull()

# 由ln(X'ni)的定义可计算(12)式的左边 ln (Xni/Xn)/(Xii/Xi)
# 可将其视为 country n's normalized import share from country i
normalized_trade_share <- -(trade_prime - trade) * beta / (1 - beta) + trade


# 六档距离,说明见P21
c(dist1, dist2, dist3, dist4, dist5, dist6) %<-% regression_data[, 6:11]

# 是否share border/language, 是否均在 EEC/EFTA 中
# 欧共体EEC是EU的前身,EFTA是欧自联
c(border, language, EU, EFTA) %<-% regression_data[, c(12, 18, 19, 20)]

# 横向合并distance, border, language, RTA 等虚拟变量
# 注意,六档距离只需要5个dummy variable
geography_dummy <- cbind(dist2, dist3, dist4, dist5, dist6, border, language, EU, EFTA)


# 以下5个变量的数值都是对数标准化的,即 ln(var_i/var_n)
# 分别是(1)R&D 支出, (2)以平均受教育年限来衡量的 human capital
# (3)人口密度, (4)制造业劳动力数量, (5)工资(均以美元计)
c(r_and_d, human_capital, density, labor, wage) %<-% regression_data[, 13:17]


# 国家首都之间的距离
distance <- regression_data$distance
ln_distance <- log(distance) # 化为对数距离


# 进口国(目的地国)虚拟变量的稀疏矩阵
destination_matrix <- kronecker(diag(N), rep(1, N)) # 克罗内克积
destination_matrix %>%
  as.data.table() %>%
  set_colnames(1:19 %>% str_c("m", .))
# 出口国(来源国)虚拟变量的稀疏矩阵
source_matrix <- kronecker(rep(1, N), diag(N))
source_matrix %>%
  as.data.table() %>%
  set_colnames(1:19 %>% str_c("S", .))
# 来源国虚拟变量 S_i-S_n, (28)式
source_dummy <- source_matrix - destination_matrix
# 这个减法决定了 source_dummy 和 destination_dummy 在(30)式中是不对称的
source_dummy %>% as.data.table() # 观察一下全貌
# 目的地国虚拟变量 m_n, (29)式
destination_dummy <- destination_matrix

# 虚拟变量多一个自由度,要以其中一个为基准
# 用其他虚拟变量与这个基准的相对差异,作为回归模型的自变量
# 以美国(第19列)为基准,前18列都减去19列
relative_source_dummy <- (source_dummy[, -N] - source_dummy[, N]) %>%
  as.data.table() %>% # 矩阵转换为DT
  set_colnames(1:18 %>% str_c("S", .))
relative_source_dummy # 观察一下全貌
relative_destination_dummy <- (destination_dummy[, -N] - destination_dummy[, N]) %>%
  as.data.table() %>%
  set_colnames(1:18 %>% str_c("m", .))
relative_destination_dummy # 观察一下全貌
## price.csv

# 50种商品的对数标准化价格(以美国为基准)
price <- price_table %>%
  select(-country) %>%
  as.matrix()


# 目的地国50种商品对数标准化价格 ln p_n(j)
destination_price <- kronecker(price, rep(1, N))
# 来源地国50种商品对数标准化价格 ln p_i(j)
source_price <- kronecker(rep(1, N), price)
# r_{ni}(j)=ln p_n(j)-ln p_i(j)
relative_price <- destination_price - source_price
# 各行最大的r_{ni}(j)
max_price <- apply(relative_price, 1, max)
# 各行最大r_{ni}(j)的j(商品种类index)
max_price_index <- apply(relative_price, 1, which.max)
# 遍历各行,将最大的r_{ni}(j)替换为-100
for (k in 1:nrow(relative_price)) {
  relative_price[k, max_price_index[k]] <- -100
}
# 然后求各行第二大的r_{ni}(j),作为作为ln d_{ni}的代理变量
ln_dni <- max_price2 <- apply(relative_price, 1, max)


# 价格指数
# 用50种商品对数标准化价格的平均值作为各国价格指数的代理变量
mean_price <- apply(price, 1, mean)
# 目的地国价格指数 ln p_n
destination_price_index <- kronecker(mean_price, rep(1, N))
# 来源地国价格指数 ln p_i
source_price_index <- kronecker(rep(1, N), mean_price)
# (13)式: D_{ni}=ln(p_i)-ln(p_n)+ln(d_{ni})
Dni <- source_price_index - destination_price_index + ln_dni
## delete invalid observations

# 删掉 n==i 的行,保留342行
# 因为这些行自变量和因变量的标准化值都等于0,属于无效数据

# 无效行的index
invalid_line_index <- which(import_country == export_country)

# destinations and sources index
import_country_valid <- import_country[-invalid_line_index]
export_country_valid <- export_country[-invalid_line_index]

# ln (Xni/Xn)/(Xii/Xi)
normalized_trade_share_valid <- normalized_trade_share[-invalid_line_index]

# ln(X'ni/X'nn)
trade_prime_valid <- trade_prime[-invalid_line_index]

# D_{ni}
Dni_valid <- Dni[-invalid_line_index]

# exp(D_{ni}),用于 Figure 2
price_measure <- exp(Dni_valid)

# ln_distance
ln_distance_valid <- ln_distance[-invalid_line_index]

# 合并距离、边界、语言、RTA等虚拟变量
geography_dummy_valid <- geography_dummy[-invalid_line_index, ]

# destinations and sources dummies 组合为数据框
relative_source_dummy_valid <- relative_source_dummy[-invalid_line_index, ]
relative_dest_dummy_valid <- relative_destination_dummy[-invalid_line_index, ]

country_dummy_valid <- cbind(
  relative_dest_dummy_valid,
  relative_source_dummy_valid
) %>% as.data.table()

Section 3

FIGURE I

# 标准化贸易份额的最大值
exp(normalized_trade_share_valid) %>% max()
#> [1] 0.3584898
# 横跨近四个数量级
exp(normalized_trade_share_valid) %>%
  max() %>%
  `/`(exp(normalized_trade_share_valid) %>% min()) %>%
  log() %>%
  `/`(log(10))
#> [1] 3.985887

FIGURE II

# 相关系数 correlation
cor(Dni_valid, normalized_trade_share_valid)
#> [1] -0.4041783

TABLE II

price_measure_table <- # 三列:进口国index,出口国index,exp(Dni)
  cbind(import_country_valid, export_country_valid, price_measure) %>%
  as.data.table() %>% # 转换数据类型
  # 左连接匹配国家代码(code列)
  left_join(country_table, by = c("import_country_valid" = "id")) %>%
  rename(dest = code) %>%
  left_join(country_table, by = c("export_country_valid" = "id")) %>%
  rename(source = code) %>%
  # 挑选这三列,其余删掉
  select(dest, source, price_measure)

price_measure_table
table2 <- country_table$code %>% # 迭代对象: 19个国家代码
  map_dfr( # 每轮迭代生成一行,最后把这些行纵向摞起来
    function(country_code) {

      # select 进口国为country_code的所有的行
      dest_table <- price_measure_table[dest == country_code, ]

      source_min <- dest_table[
        which.min(price_measure), # select price_measure 最小值所在的行
      ][
        , concatenation := str_c(source, "(", sprintf("%0.2f", price_measure), ")")
      ] %>% pull(concatenation)

      source_max <- dest_table[
        which.max(price_measure),
      ][
        , concatenation := str_c(source, "(", sprintf("%0.2f", price_measure), ")")
      ] %>% pull(concatenation)

      # 出口国为country_code的所有的行
      source_table <- price_measure_table[source == country_code, ]

      dest_min <- source_table[
        which.min(price_measure),
      ][
        , concatenation := str_c(dest, "(", sprintf("%0.2f", price_measure), ")")
      ] %>% pull(concatenation)

      dest_max <- source_table[
        which.max(price_measure),
      ][
        , concatenation := str_c(dest, "(", sprintf("%0.2f", price_measure), ")")
      ] %>% pull(concatenation)

      # map_dfr()的每个返回值都是Table II的一行
      data.table(
        Country = str_c(
          country_table[code == country_code, ] %>% pull(name),
          " (", country_code, ")"
        ),
        source_min, source_max, dest_min, dest_max
      )
    }
  )

table2 %>%
  set_colnames(c("Country", "Minimum", "Maximum", "Minimum", "Maximum")) %>%
  prettify(caption = "TABLE II \\\n Price Measure Statistics") %>%
  add_header_above(c(" " = 1, "Foreign Source \n (Column 1 As Destination)" = 2, "Foreign Destinations \n (Column 1 As Source)" = 2)) %>%
  footnote(
    general = "本表中的数值为 $e^{D_{ni}}$,其中 $D_{ni}$ 在 (13) 式中定义,为 $\\ln (p_i d_{ni}/p_n)$ 的代理变量。因此,$e^{D_{ni}}$ 表示进口国 $n$ 若全部从出口国 $i$ 的市场购买商品(花费当地价格及运输成本),比实际的购买(在本国市场充分遵循比较优势)会贵多少。",
    general_title = "\n Note: ",
    footnote_as_chunk = T
  )
TABLE II
Price Measure Statistics
Foreign Source
(Column 1 As Destination)
Foreign Destinations
(Column 1 As Source)
Country Minimum Maximum Minimum Maximum
Australia (AL) NE(1.44) PO(2.25) BE(1.41) US(2.03)
Austria (AU) SW(1.39) NZ(2.16) UK(1.47) JP(1.97)
Belgium (BE) GE(1.25) JP(2.02) GE(1.35) SW(1.77)
Canada (CA) US(1.58) NZ(2.57) AU(1.57) US(2.14)
Denmark (DK) FI(1.36) PO(2.21) NE(1.48) US(2.41)
Finland (FI) SW(1.38) PO(2.61) DK(1.36) US(2.87)
France (FR) GE(1.33) NZ(2.42) BE(1.40) JP(2.40)
Germany (GE) BE(1.35) NZ(2.28) BE(1.25) US(2.22)
Greece (GR) SP(1.61) NZ(2.71) NE(1.48) US(2.27)
Italy (IT) FR(1.45) NZ(2.19) AU(1.46) JP(2.10)
Japan (JP) BE(1.62) PO(3.25) AL(1.72) US(3.08)
Netherlands (NE) GE(1.30) NZ(2.17) DK(1.39) NZ(2.01)
New Zealand (NZ) CA(1.60) PO(2.08) AL(1.64) GR(2.71)
Norway (NO) FI(1.45) JP(2.84) SW(1.36) US(2.31)
Portugal (PO) BE(1.49) JP(2.56) SP(1.59) JP(3.25)
Spain (SP) BE(1.39) JP(2.47) NO(1.51) JP(3.05)
Sweden (SW) NO(1.36) US(2.70) FI(1.38) US(2.01)
United Kingdom (UK) NE(1.46) JP(2.37) FR(1.52) NZ(2.04)
United States (US) FR(1.57) JP(3.08) CA(1.58) SW(2.70)

Note:
本表中的数值为 \(e^{D_{ni}}\),其中 \(D_{ni}\) 在 (13) 式中定义,为 \(\ln (p_i d_{ni}/p_n)\) 的代理变量。因此,\(e^{D_{ni}}\) 表示进口国 \(n\) 若全部从出口国 \(i\) 的市场购买商品(花费当地价格及运输成本),比实际的购买(在本国市场充分遵循比较优势)会贵多少。

用 (12) 式估计 \(\theta\)

\(\ln (Xni/Xn)/(Xii/Xi)\) 为被解释变量,以 \(D_{ni}\) 为解释变量,估计出来的系数是 \(-\theta\),因此 \(\theta\) 值还要取一个负号。

Moments Estimation

最简单的一阶矩估计

x_center <- mean(Dni_valid)
y_center <- mean(normalized_trade_share_valid)
theta <- y_center / x_center
theta
#> [1] -8.27593

\(\theta=8.28\)

OLS Estimation

# 无截距项
lm_1 <- lm(normalized_trade_share_valid ~ 0 + Dni_valid)
summary(lm_1) %>%
  `[[`("coefficients") %>%
  prettify()
Estimate Std. Error t value Pr(>|t|)
Dni_valid -8.025323 0.1542 -52.04491 0

\(\theta=8.03(0.15)\), 与矩估计的估计值很接近。

# 有截距项
lm_2 <- lm(normalized_trade_share_valid ~ Dni_valid)
summary(lm_2) %>%
  `[[`("coefficients") %>%
  prettify()
Estimate Std. Error t value Pr(>|t|)
(Intercept) -2.173133 0.3409387 -6.373971 0
Dni_valid -4.571893 0.5611163 -8.147851 0

\(\theta=4.57(0.56)\). 截距项为负,与理论预测(为0)不一致,表明数据中可能有较大的误差.

分别估计 \(D_{ni}\) 三个组成部分的参数

探讨 \(D_{ni}\) 三个组成部分 \(\ln p_i, \ln p_n, \ln d_{ni}\) 对标准化贸易份额的分别贡献。

# 三个组成部分分别为三列,去掉无效行
trade_share_components <- data.table(
  y = normalized_trade_share_valid,
  ln_pi = source_price_index[-invalid_line_index],
  ln_pn = destination_price_index[-invalid_line_index],
  ln_dni = ln_dni[-invalid_line_index]
)

# 无截距项
lm_3 <- lm(y ~ 0 + ln_pi + ln_pn + ln_dni, data = trade_share_components)
summary(lm_3) %>%
  `[[`("coefficients") %>%
  prettify()
Estimate Std. Error t value Pr(>|t|)
ln_pi -9.044924 0.4755234 -19.020987 0
ln_pn 6.350751 0.8031414 7.907389 0
ln_dni -6.837406 0.3272661 -20.892493 0
# 有截距项
lm_4 <- lm(y ~ ln_pi + ln_pn + ln_dni, data = trade_share_components)
summary(lm_4) %>%
  `[[`("coefficients") %>%
  prettify()
Estimate Std. Error t value Pr(>|t|)
(Intercept) -2.358243 0.5254622 -4.487940 9.9e-06
ln_pi -4.878989 1.0371534 -4.704211 3.7e-06
ln_pn 5.488339 0.8046659 6.820644 0.0e+00
ln_dni -4.555882 0.5998471 -7.595072 0.0e+00

无论有无截距项,估计出来的参数的正负与理论预测的一致

IV Estimation

有截距 OLS 回归的截距不为0,表明我们的价格数据可能有系统误差。

为 price measure \(D_{ni}\) 寻找工具变量(IV),用工具变量法估计 \(\theta\) (以下两种估计仅在源代码中出现,未在论文中出现).

  1. 以对数实际距离作为 \(D_{ni}\) 的工具变量
# ivreg::ivreg() 可以做工具变量回归,第一个参数(字符串)为回归公式,形式为:
# 被解释变量 ~ 内生变量 + 外生变量 | 工具变量 + 外生变量
fit_iv_1 <- ivreg(normalized_trade_share_valid ~ Dni_valid | ln_distance_valid)
summary(fit_iv_1, test = TRUE) # 对IV回归进行诊断
#> 
#> Call:
#> ivreg(formula = normalized_trade_share_valid ~ Dni_valid | ln_distance_valid)
#> 
#> Residuals:
#>     Min      1Q  Median      3Q     Max 
#> -6.2553 -1.6047 -0.2018  1.1491  9.1736 
#> 
#> Coefficients:
#>             Estimate Std. Error t value Pr(>|t|)    
#> (Intercept)   3.6579     0.9311   3.929 0.000104 ***
#> Dni_valid   -14.5108     1.5732  -9.224  < 2e-16 ***
#> 
#> Diagnostic tests:
#>                  df1 df2 statistic p-value    
#> Weak instruments   1 340     110.1  <2e-16 ***
#> Wu-Hausman         1 339     144.5  <2e-16 ***
#> Sargan             0  NA        NA      NA    
#> ---
#> Signif. codes:  0 '***' 0.001 '**' 0.01 '*' 0.05 '.' 0.1 ' ' 1
#> 
#> Residual standard error: 2.274 on 340 degrees of freedom
#> Multiple R-Squared: -0.6087, Adjusted R-squared: -0.6134 
#> Wald test: 85.08 on 1 and 340 DF,  p-value: < 2.2e-16

IV 回归通过了诊断,\(\theta=14.51(1.57)\)

  1. 以地理距离、source1 & destination dummies 作为 \(D_{ni}\) 的工具变量
instrument_data <- cbind(ln_distance_valid, country_dummy_valid)
formula_instrument <- colnames(instrument_data) %>% str_c(collapse = " + ")
formula_instrument
#> [1] "ln_distance_valid + m1 + m2 + m3 + m4 + m5 + m6 + m7 + m8 + m9 + m10 + m11 + m12 + m13 + m14 + m15 + m16 + m17 + m18 + S1 + S2 + S3 + S4 + S5 + S6 + S7 + S8 + S9 + S10 + S11 + S12 + S13 + S14 + S15 + S16 + S17 + S18"
fit_iv_2 <- ivreg(
  formula = str_c("normalized_trade_share_valid ~ Dni_valid | ", formula_instrument),
  data = cbind(normalized_trade_share_valid, Dni_valid, instrument_data)
)
summary(fit_iv_2, test = TRUE)
#> 
#> Call:
#> ivreg(formula = str_c("normalized_trade_share_valid ~ Dni_valid | ", 
#>     formula_instrument), data = cbind(normalized_trade_share_valid, 
#>     Dni_valid, instrument_data))
#> 
#> Residuals:
#>      Min       1Q   Median       3Q      Max 
#> -5.19771 -1.18245 -0.03927  1.19787  5.08399 
#> 
#> Coefficients:
#>             Estimate Std. Error t value Pr(>|t|)    
#> (Intercept)  -0.8079     0.4281  -1.887     0.06 .  
#> Dni_valid    -6.8989     0.7130  -9.676   <2e-16 ***
#> 
#> Diagnostic tests:
#>                  df1 df2 statistic  p-value    
#> Weak instruments  37 304     15.30  < 2e-16 ***
#> Wu-Hausman         1 339     35.26 7.15e-09 ***
#> Sargan            36  NA    263.45  < 2e-16 ***
#> ---
#> Signif. codes:  0 '***' 0.001 '**' 0.01 '*' 0.05 '.' 0.1 ' ' 1
#> 
#> Residual standard error: 1.681 on 340 degrees of freedom
#> Multiple R-Squared: 0.121,   Adjusted R-squared: 0.1185 
#> Wald test: 93.62 on 1 and 340 DF,  p-value: < 2.2e-16

\(\theta=6.90(0.71)\)

Section 5.3

估计一个结果被报告在正文中、但方程从未出现过的计量模型2:以 \(\ln (X'_{ni}/X'_{nn})\) 为被解释变量,\(D_{ni}\) 为内生解释变量,source & destination dummies 为外生解释变量

OLS Estimation

lm_5 <- lm(
  trade_prime_valid ~ ., # . 代表所有其他变量
  data = cbind(trade_prime_valid, Dni_valid, country_dummy_valid)
)
summary(lm_5) %>%
  `[[`("coefficients") %>%
  prettify()
Estimate Std. Error t value Pr(>|t|)
(Intercept) -3.4199162 0.2933648 -11.6575540 0.0000000
Dni_valid -2.4467276 0.4931804 -4.9611210 0.0000012
m1 -3.0808876 0.3050435 -10.0998319 0.0000000
m2 -0.9392800 0.3064023 -3.0655128 0.0023680
m3 1.7171125 0.3210312 5.3487408 0.0000002
m4 -1.4324888 0.2989970 -4.7909809 0.0000026
m5 0.2877993 0.3039180 0.9469635 0.3444095
m6 -0.5447744 0.2988159 -1.8231105 0.0692687
m7 1.2016105 0.3008315 3.9942971 0.0000814
m8 2.0422942 0.3060856 6.6722978 0.0000000
m9 -1.6337823 0.3039547 -5.3750855 0.0000002
m10 0.4851516 0.3055756 1.5876645 0.1134017
m11 -0.4603440 0.3458418 -1.3310826 0.1841592
m12 1.8317076 0.3058050 5.9897889 0.0000000
m13 -2.2669667 0.3286080 -6.8986952 0.0000000
m14 0.0388581 0.2987892 0.1300520 0.8966113
m15 -0.3173925 0.3118610 -1.0177370 0.3096122
m16 -0.7589797 0.3012969 -2.5190428 0.0122802
m17 1.0137428 0.2987878 3.3928520 0.0007833
m18 1.8161109 0.3006685 6.0402427 0.0000000
S1 -1.4140555 0.2066347 -6.8432638 0.0000000
S2 -0.7551922 0.2073354 -3.6423696 0.0003175
S3 -3.0754706 0.2161052 -14.2313592 0.0000000
S4 -0.7201263 0.2058235 -3.4987570 0.0005373
S5 -1.3617033 0.2077610 -6.5541802 0.0000000
S6 -0.1235467 0.2056388 -0.6007946 0.5484244
S7 1.7854210 0.2061861 8.6592711 0.0000000
S8 2.8383352 0.2095910 13.5422546 0.0000000
S9 -2.4888271 0.2066605 -12.0430736 0.0000000
S10 1.9614312 0.2090452 9.3828110 0.0000000
S11 3.1925417 0.2246246 14.2127856 0.0000000
S12 -1.7780664 0.2082723 -8.5372199 0.0000000
S13 -2.1422594 0.2347276 -9.1265782 0.0000000
S14 -0.9624557 0.2075509 -4.6372043 0.0000053
S15 -0.9158288 0.2234968 -4.0977259 0.0000536
S16 0.5262126 0.2061498 2.5525743 0.0111817
S17 0.4185237 0.2070864 2.0210099 0.0441550
S18 1.8218525 0.2074390 8.7825923 0.0000000

\(\theta=2.45(0.49)\)

IV Estimation

以 geography_dummies 为工具变量,包括距离、边界、语言、RTA 等,解释内生变量 D_ni;country_dummies 为外生变量。

TSLS_data <- cbind(trade_prime_valid, Dni_valid, geography_dummy_valid, country_dummy_valid)
TSLS_data
# 外生变量
formula_exogenous <- colnames(country_dummy_valid) %>% str_c(collapse = " + ")
formula_exogenous
#> [1] "m1 + m2 + m3 + m4 + m5 + m6 + m7 + m8 + m9 + m10 + m11 + m12 + m13 + m14 + m15 + m16 + m17 + m18 + S1 + S2 + S3 + S4 + S5 + S6 + S7 + S8 + S9 + S10 + S11 + S12 + S13 + S14 + S15 + S16 + S17 + S18"
# 工具变量
formula_instrument <- colnames(geography_dummy_valid) %>% str_c(collapse = " + ")
formula_instrument
#> [1] "dist2 + dist3 + dist4 + dist5 + dist6 + border + language + EU + EFTA"
# 回归公式
formula <- str_c(
  "trade_prime_valid ~ Dni_valid + ", formula_exogenous, " | ",
  formula_instrument, " + ", formula_exogenous
)
formula
#> [1] "trade_prime_valid ~ Dni_valid + m1 + m2 + m3 + m4 + m5 + m6 + m7 + m8 + m9 + m10 + m11 + m12 + m13 + m14 + m15 + m16 + m17 + m18 + S1 + S2 + S3 + S4 + S5 + S6 + S7 + S8 + S9 + S10 + S11 + S12 + S13 + S14 + S15 + S16 + S17 + S18 | dist2 + dist3 + dist4 + dist5 + dist6 + border + language + EU + EFTA + m1 + m2 + m3 + m4 + m5 + m6 + m7 + m8 + m9 + m10 + m11 + m12 + m13 + m14 + m15 + m16 + m17 + m18 + S1 + S2 + S3 + S4 + S5 + S6 + S7 + S8 + S9 + S10 + S11 + S12 + S13 + S14 + S15 + S16 + S17 + S18"
fit_iv_3 <- ivreg(formula = formula, data = TSLS_data)
summary(fit_iv_3, test = TRUE)
#> 
#> Call:
#> ivreg(formula = formula, data = TSLS_data)
#> 
#> Residuals:
#>      Min       1Q   Median       3Q      Max 
#> -4.03108 -0.87353 -0.07295  0.91475  5.54823 
#> 
#> Coefficients:
#>               Estimate Std. Error t value Pr(>|t|)    
#> (Intercept)   2.690744   1.021376   2.634 0.008860 ** 
#> Dni_valid   -12.862154   1.736076  -7.409 1.27e-12 ***
#> m1           -4.379061   0.516788  -8.474 1.04e-15 ***
#> m2           -2.373090   0.526655  -4.506 9.44e-06 ***
#> m3           -0.762720   0.625382  -1.220 0.223560    
#> m4           -1.195235   0.470969  -2.538 0.011654 *  
#> m5           -0.886755   0.508505  -1.744 0.082197 .  
#> m6           -0.634263   0.469543  -1.351 0.177761    
#> m7            0.461957   0.485230   0.952 0.341834    
#> m8            0.638974   0.524368   1.219 0.223956    
#> m9           -0.455004   0.508776  -0.894 0.371863    
#> m10          -0.867693   0.520670  -1.666 0.096645 .  
#> m11           3.217836   0.772093   4.168 4.02e-05 ***
#> m12           0.455939   0.522336   0.873 0.383415    
#> m13           0.621791   0.672382   0.925 0.355825    
#> m14           0.008904   0.469333   0.019 0.984876    
#> m15           1.569687   0.564966   2.778 0.005803 ** 
#> m16          -1.578771   0.488795  -3.230 0.001374 ** 
#> m17           0.990810   0.469322   2.111 0.035575 *  
#> m18           1.106633   0.483976   2.287 0.022910 *  
#> S1           -1.842036   0.330782  -5.569 5.65e-08 ***
#> S2           -1.314255   0.336172  -3.909 0.000114 ***
#> S3           -4.478607   0.398783 -11.231  < 2e-16 ***
#> S4           -0.904355   0.324455  -2.787 0.005649 ** 
#> S5           -1.987282   0.339413  -5.855 1.24e-08 ***
#> S6           -0.116991   0.323000  -0.362 0.717454    
#> S7            1.468290   0.327295   4.486 1.03e-05 ***
#> S8            1.982772   0.353079   5.616 4.42e-08 ***
#> S9           -2.055326   0.330982  -6.210 1.74e-09 ***
#> S10           1.167665   0.349046   3.345 0.000925 ***
#> S11           5.101323   0.453382  11.252  < 2e-16 ***
#> S12          -2.475357   0.343273  -7.211 4.43e-12 ***
#> S13           0.247988   0.512895   0.484 0.629084    
#> S14          -1.556102   0.337816  -4.606 6.03e-06 ***
#> S15           0.932966   0.446422   2.090 0.037460 *  
#> S16           0.219792   0.327012   0.672 0.502017    
#> S17          -0.097743   0.334265  -0.292 0.770172    
#> S18           1.245900   0.336963   3.697 0.000258 ***
#> 
#> Diagnostic tests:
#>                  df1 df2 statistic  p-value    
#> Weak instruments   9 296     8.176 7.44e-11 ***
#> Wu-Hausman         1 303   173.953  < 2e-16 ***
#> Sargan             8  NA    47.419 1.28e-07 ***
#> ---
#> Signif. codes:  0 '***' 0.001 '**' 0.01 '*' 0.05 '.' 0.1 ' ' 1
#> 
#> Residual standard error: 1.406 on 304 degrees of freedom
#> Multiple R-Squared: 0.7955,  Adjusted R-squared: 0.7706 
#> Wald test: 38.05 on 37 and 304 DF,  p-value: < 2.2e-16

\(\theta=12.86(1.74)\)

Section 5.1

TABLE III

估计 (30) 式

OLS estimation

# 组织数据框
table3_data <- cbind(
  trade_prime, dist1, geography_dummy,
  relative_source_dummy, relative_destination_dummy
) %>%
  as.data.table() %>%
  `[`(-invalid_line_index, )

# OLS
lm_table3 <- lm(trade_prime ~ 0 + ., data = table3_data)
summary(lm_table3)
#> 
#> Call:
#> lm(formula = trade_prime ~ 0 + ., data = table3_data)
#> 
#> Residuals:
#>      Min       1Q   Median       3Q      Max 
#> -1.37812 -0.28260  0.00324  0.27485  1.35971 
#> 
#> Coefficients:
#>           Estimate Std. Error t value Pr(>|t|)    
#> dist1    -3.102440   0.154903 -20.028  < 2e-16 ***
#> dist2    -3.665941   0.106969 -34.271  < 2e-16 ***
#> dist3    -4.033395   0.095713 -42.141  < 2e-16 ***
#> dist4    -4.218077   0.153080 -27.555  < 2e-16 ***
#> dist5    -6.064372   0.087005 -69.701  < 2e-16 ***
#> dist6    -6.558933   0.097792 -67.070  < 2e-16 ***
#> border    0.303564   0.137159   2.213 0.027645 *  
#> language  0.510080   0.145505   3.506 0.000526 ***
#> EU        0.035912   0.121613   0.295 0.767974    
#> EFTA      0.536071   0.182563   2.936 0.003581 ** 
#> S1        0.192558   0.149741   1.286 0.199471    
#> S2       -1.161839   0.128054  -9.073  < 2e-16 ***
#> S3       -3.335625   0.118827 -28.071  < 2e-16 ***
#> S4        0.411561   0.141915   2.900 0.004010 ** 
#> S5       -1.749550   0.121735 -14.372  < 2e-16 ***
#> S6       -0.522466   0.129777  -4.026 7.22e-05 ***
#> S7        1.281384   0.118952  10.772  < 2e-16 ***
#> S8        2.352748   0.121609  19.347  < 2e-16 ***
#> S9       -2.813521   0.122484 -22.971  < 2e-16 ***
#> S10       1.781510   0.120437  14.792  < 2e-16 ***
#> S11       4.198787   0.132413  31.710  < 2e-16 ***
#> S12      -2.189319   0.120839 -18.118  < 2e-16 ***
#> S13      -1.197687   0.149741  -7.998 2.87e-14 ***
#> S14      -1.346152   0.129424 -10.401  < 2e-16 ***
#> S15      -1.573180   0.126130 -12.473  < 2e-16 ***
#> S16       0.303089   0.121268   2.499 0.012984 *  
#> S17       0.009816   0.129869   0.076 0.939800    
#> S18       1.374167   0.121654  11.296  < 2e-16 ***
#> m1        0.236221   0.256161   0.922 0.357197    
#> m2       -1.678415   0.203764  -8.237 5.75e-15 ***
#> m3        1.120118   0.180023   6.222 1.67e-09 ***
#> m4        0.688596   0.237671   2.897 0.004045 ** 
#> m5       -0.505889   0.187633  -2.696 0.007416 ** 
#> m6       -1.334488   0.207808  -6.422 5.36e-10 ***
#> m7        0.218294   0.180352   1.210 0.227099    
#> m8        0.998812   0.187305   5.333 1.93e-07 ***
#> m9       -2.356411   0.189573 -12.430  < 2e-16 ***
#> m10       0.070178   0.184252   0.381 0.703566    
#> m11       1.584890   0.214620   7.385 1.56e-12 ***
#> m12       1.004782   0.185301   5.422 1.22e-07 ***
#> m13       0.066574   0.256161   0.260 0.795129    
#> m14      -1.000409   0.207199  -4.828 2.21e-06 ***
#> m15      -1.206780   0.198907  -6.067 3.97e-09 ***
#> m16      -1.156611   0.186420  -6.204 1.85e-09 ***
#> m17      -0.024864   0.208183  -0.119 0.905012    
#> m18       0.816808   0.187422   4.358 1.81e-05 ***
#> ---
#> Signif. codes:  0 '***' 0.001 '**' 0.01 '*' 0.05 '.' 0.1 ' ' 1
#> 
#> Residual standard error: 0.4913 on 296 degrees of freedom
#> Multiple R-squared:  0.9935, Adjusted R-squared:  0.9925 
#> F-statistic: 984.2 on 46 and 296 DF,  p-value: < 2.2e-16

GLS estimation

  • 由理论推断,(30) 式的回归模型违反了 OLS 的基本假设: \(\text{cov}(\varepsilon_j, \varepsilon_k)=E(\varepsilon_{j}\varepsilon_{k})-E(\varepsilon_{j})E(\varepsilon_{k})=E(\varepsilon_{j}\varepsilon_{k}) = 0, \forall j \neq k\).

    • 这是因为,贸易具有互惠性,如果 \(i\) 国向 \(n\) 国出口的贸易障碍偏低(实际值低于模型拟合值),则一般 \(n\) 国向 \(i\) 国出口的贸易障碍也会偏低。这两个误差 \(\varepsilon_{n \leftarrow i}, \varepsilon_{i\leftarrow n}\)(以下简写为 \(\varepsilon_{ni}\)\(\varepsilon_{in}\))往往同时偏高或偏低,有一定相关性,故 \(\text{cov}(\varepsilon_{ni}, \varepsilon_{in})>0\)

    • 设误差 \(\varepsilon_{ni}=\varepsilon_{ni}^1+\varepsilon_{ni}^2\) 可以分为两部分,两部分之间不相关

    • 第一部分 \(\varepsilon_{ni}^1\) 符合 OLS 的经典假设,即 \(\begin{aligned}E(\varepsilon_{ab}^1\varepsilon_{cd}^1) = \left\{\begin{matrix} \sigma_1^2, & \forall a=c \land b=d\\ 0, & \text{otherwise.} \end{matrix}\right.\end{aligned}\)

    • 第二部分专门体现两国贸易的互惠性,有性质 \(\varepsilon_{ni}^2=\varepsilon_{in}^2\),使得 \(E(\varepsilon_{ni}^2\varepsilon_{in}^2)= E(\varepsilon_{ni}^2\varepsilon_{ni}^2) =\sigma_2^2\)

    • 则总误差满足 \[\begin{align} E(\varepsilon_{ab}\varepsilon_{cd}) & = E(\varepsilon_{ab}^1\varepsilon_{cd}^1)+E(\varepsilon_{ab}^1\varepsilon_{cd}^2)+E(\varepsilon_{ab}^2\varepsilon_{cd}^1)+E(\varepsilon_{ab}^2\varepsilon_{cd}^2) \\ &=E(\varepsilon_{ab}^1\varepsilon_{cd}^1)+E(\varepsilon_{ab}^2\varepsilon_{cd}^2) \\ &= \left\{\begin{matrix} \sigma_1^2+\sigma_2^2, & \forall a=c \land b=d \\ \sigma_2^2, & \forall a=d \land b=c\\ 0, & \text{otherwise.} \end{matrix}\right. \end{align}\]

  • 误差项有了上述性质,便不能再使用 OLS estimation,而应使用广义最小二乘法(GLS)3

    • 设误差向量 \(\boldsymbol{\varepsilon}\) 的协方差矩阵为 \(\boldsymbol{\Omega}\),则系数向量 \(\boldsymbol{\beta}\) 在经过一定变换后的新模型中的 GLS estimator 为 \(\hat{\boldsymbol{\beta}}^\ast=(\boldsymbol{X}'\boldsymbol{\Omega}^{-1}\boldsymbol{X})^{-1}\boldsymbol{X}'\boldsymbol{\Omega}^{-1}\boldsymbol{Y}\),协方差矩阵为 \(\text{Var}(\hat{\boldsymbol{\beta}}^\ast)=(\boldsymbol{X}'\boldsymbol{\Omega}^{-1}\boldsymbol{X})^{-1}\)
    • 事实上,\(\boldsymbol{\Omega}\) 的具体形式是很难了解的。但在本文中,可以根据理论,使用 \(\boldsymbol{e}\boldsymbol{e}'\) 对其进行估计(\(\boldsymbol{e}\) 为残差向量)
  • 对于纯粹的异方差问题(误差的协方差矩阵只是对角元素不同,但非对角元素保证为 0),R base 中有 lm()lm.gls() 函数可以直接用;但对于协方差矩阵非对角元素不为零的情况,目前似乎没有很好的 library 提供现成的函数,需要自己写矩阵运算。

# 由 OLS 求得所有观测的残差,并将其扩展为矩阵,作为估计误差协方差的材料
ee_matrix <- lm_table3$residuals %o% lm_table3$residuals
# 这是一个 342*342 的大矩阵

# 估计 sigma_1^2 + sigma_2^2
sum_sigma_square <- diag(ee_matrix) %>% # 从n到i与从n到i的trade_prime的残差之积
  mean() # 期望为 sigma_1^2 + sigma_2^2

# 估计 sigma_2^2
observation_valid <- data.table(n = import_country, i = export_country) %>%
  `[`(-invalid_line_index, ) %>%
  `[`(, row_index := .I)

print(observation_valid)
#>       n  i row_index
#>   1:  1  2         1
#>   2:  1  3         2
#>   3:  1  4         3
#>   4:  1  5         4
#>   5:  1  6         5
#>  ---                
#> 338: 19 14       338
#> 339: 19 15       339
#> 340: 19 16       340
#> 341: 19 17       341
#> 342: 19 18       342
sigma2_square <- observation_valid$row_index %>%
  map_dbl(function(row_index) {
    row_n <- observation_valid$n[row_index]
    row_i <- observation_valid$i[row_index]
    col_index <- observation_valid[n == row_i & i == row_n, ]$row_index
    ee_matrix[row_index, col_index] # 从n到i与从i到n的trade_prime的残差之积
  }) %>%
  mean() # 期望为 sigma_2^2

sigma2_square
#> [1] 0.05064993
sum_sigma_square - sigma2_square
#> [1] 0.1582666

因此

\(\theta^2\sigma_2^2=\) 0.05

\(\theta^2\sigma_1^2=\) 0.16

# 误差协方差矩阵 Omega
Omega <- diag(nrow(observation_valid)) * sum_sigma_square

observation_valid$row_index %>%
  walk(function(row_index) {
    row_n <- observation_valid$n[row_index]
    row_i <- observation_valid$i[row_index]
    col_index <- observation_valid[n == row_i & i == row_n, ]$row_index
    Omega[row_index, col_index] <<- sigma2_square # "<<-" 对环境外变量赋值
  })

Omega %>% round(2) %>% as.data.table()
# 求逆
Omega_inverse <- solve(Omega)

# GLS estimation
Y <- table3_data$trade_prime
X <- table3_data[, -1] %>% as.matrix()

estimate <- solve(t(X) %*% Omega_inverse %*% X) %*% t(X) %*% Omega_inverse %*% Y
estimate_S19 <- -estimate[11:28] %>% sum() # 保证虚拟变量效应之和为0
estimate_m19 <- -estimate[29:46] %>% sum()

var_estimate <- solve(t(X) %*% Omega_inverse %*% X)
stand_error <- diag(var_estimate) %>% sqrt()
stand_error_S19 <- var_estimate[11:28, 11:28] %>%
  sum() %>% # -S19等于S1到S18的和,因此S19的方差应等于S1到S18所有的方差和协方差之和
  sqrt()
stand_error_m19 <- var_estimate[29:46, 29:46] %>%
  sum() %>%
  sqrt()
# Table III
gls_estimate <- c(
  estimate[1:28], estimate_S19,
  estimate[29:46], estimate_m19
)
gls_stand_error <- c(
  stand_error[1:28], stand_error_S19,
  stand_error[29:46], stand_error_m19
)
gls_parameters <- c(
  1:6 %>% str_c("$-\\theta d_{", ., "}$"),
  "$-\\theta b$", "$-\\theta l$", "$-\\theta e_1$", "$-\\theta e_2$",
  1:19 %>% str_c("$S_{", ., "}$"),
  1:19 %>% str_c("$-\\theta m_{", ., "}$")
)
variable_names <- c(
  "Distance [0, 375)", "Distance [375, 750)", "Distance [750, 1500)",
  "Distance [1500, 3000)", "Distance [3000, 6000)", "Distance [6000, maximum)",
  "Shared border", "Shared language", "Both in EEC/EU", "Both in EFTA",
  country_table$name %>% str_c("Source country: ", .),
  country_table$name %>% str_c("Destination country: ", .)
)


table3 <- data.table(
  variables = variable_names,
  parameters = gls_parameters,
  estimate = round(gls_estimate, 2),
  std_error = round(gls_stand_error, 2)
)

table3 %>%
  mutate(std_error = str_c("(", std_error, ")")) %>%
  set_colnames(c("Variable", "parameter", "est.", "s.e.")) %>%
  prettify(caption = "TABLE III \\\n Bilateral Trade Equation") %>%
  footnote(
    general = "Estimated by GLS. The parameter are normalized so that ${\\textstyle \\sum_{i=1}^{19} S_i}=0$ and ${\\textstyle \\sum_{n=1}^{19} m_n}=0$. Standard errors are in parentheses.",
    general_title = "\n Note: ",
    footnote_as_chunk = T
  )
TABLE III
Bilateral Trade Equation
Variable parameter est. s.e.
Distance [0, 375) \(-\theta d_{1}\) -3.10 (0.16)
Distance [375, 750) \(-\theta d_{2}\) -3.66 (0.11)
Distance [750, 1500) \(-\theta d_{3}\) -4.03 (0.1)
Distance [1500, 3000) \(-\theta d_{4}\) -4.22 (0.16)
Distance [3000, 6000) \(-\theta d_{5}\) -6.06 (0.09)
Distance [6000, maximum) \(-\theta d_{6}\) -6.56 (0.1)
Shared border \(-\theta b\) 0.30 (0.14)
Shared language \(-\theta l\) 0.51 (0.15)
Both in EEC/EU \(-\theta e_1\) 0.04 (0.13)
Both in EFTA \(-\theta e_2\) 0.54 (0.19)
Source country: Australia \(S_{1}\) 0.19 (0.15)
Source country: Austria \(S_{2}\) -1.16 (0.12)
Source country: Belgium \(S_{3}\) -3.34 (0.11)
Source country: Canada \(S_{4}\) 0.41 (0.14)
Source country: Denmark \(S_{5}\) -1.75 (0.12)
Source country: Finland \(S_{6}\) -0.52 (0.12)
Source country: France \(S_{7}\) 1.28 (0.11)
Source country: Germany \(S_{8}\) 2.35 (0.12)
Source country: Greece \(S_{9}\) -2.81 (0.12)
Source country: Italy \(S_{10}\) 1.78 (0.11)
Source country: Japan \(S_{11}\) 4.20 (0.13)
Source country: Netherlands \(S_{12}\) -2.19 (0.11)
Source country: New Zealand \(S_{13}\) -1.20 (0.15)
Source country: Norway \(S_{14}\) -1.35 (0.12)
Source country: Portugal \(S_{15}\) -1.57 (0.12)
Source country: Spain \(S_{16}\) 0.30 (0.12)
Source country: Sweden \(S_{17}\) 0.01 (0.12)
Source country: United Kingdom \(S_{18}\) 1.37 (0.12)
Source country: United States \(S_{19}\) 3.98 (0.14)
Destination country: Australia \(-\theta m_{1}\) 0.24 (0.27)
Destination country: Austria \(-\theta m_{2}\) -1.68 (0.21)
Destination country: Belgium \(-\theta m_{3}\) 1.12 (0.19)
Destination country: Canada \(-\theta m_{4}\) 0.69 (0.25)
Destination country: Denmark \(-\theta m_{5}\) -0.51 (0.19)
Destination country: Finland \(-\theta m_{6}\) -1.33 (0.22)
Destination country: France \(-\theta m_{7}\) 0.22 (0.19)
Destination country: Germany \(-\theta m_{8}\) 1.00 (0.19)
Destination country: Greece \(-\theta m_{9}\) -2.36 (0.2)
Destination country: Italy \(-\theta m_{10}\) 0.07 (0.19)
Destination country: Japan \(-\theta m_{11}\) 1.59 (0.22)
Destination country: Netherlands \(-\theta m_{12}\) 1.00 (0.19)
Destination country: New Zealand \(-\theta m_{13}\) 0.07 (0.27)
Destination country: Norway \(-\theta m_{14}\) -1.00 (0.21)
Destination country: Portugal \(-\theta m_{15}\) -1.21 (0.21)
Destination country: Spain \(-\theta m_{16}\) -1.16 (0.19)
Destination country: Sweden \(-\theta m_{17}\) -0.02 (0.22)
Destination country: United Kingdom \(-\theta m_{18}\) 0.81 (0.19)
Destination country: United States \(-\theta m_{19}\) 2.46 (0.25)

Note:
Estimated by GLS. The parameter are normalized so that \({\textstyle \sum_{i=1}^{19} S_i}=0\) and \({\textstyle \sum_{n=1}^{19} m_n}=0\). Standard errors are in parentheses.

保存估计结果

TABLE III 的估计值对于下一步的 simulation 非常重要。

  1. Source country dummy 的估计值可用于计算各国技术水平
  2. 其他虚拟变量的估计值(\(-\theta \ln(d_{ni})\) 各组成部分的系数)可计算 \(-\theta \ln(d_{ni})\) 的拟合值。将此拟合值命名为 barrier_measure,作为 simulation 阶段 \(d_{ni}\) 的数据来源。
table3_estimate <- gls_estimate # 是用高精度估计值
# table3$estimate 的数据只有两位小数,不能用

barrier_dummy <- cbind(regression_data[, c(6:12, 18:20)], destination_dummy) %>%
  as.matrix() # 361*29
barrier_estimate <- gls_estimate[c(1:10, 30:48)] # 29*1

barrier_measure <- barrier_dummy %*% barrier_estimate %>% # 361*1
  `[<-`(invalid_line_index, 0) %>% # n==i 的行取0
  matrix(nrow = N, byrow = TRUE)
# 保存为 R 二进制文件 .rda,使用时直接 load()
save(table3_estimate, barrier_measure,
  file = "../data/estimation-output.rda"
)

Section 5.2

TABLE IV

# 所有国家相对于美国的 R&D stock,TABLE 4 的第一列
relative_r_and_d <- exp(r_and_d[1:N]) / exp(r_and_d[N])
# 各国平均教育年限,TABLE 4 的第二列
edu_year <- regression_data[1:N, 22][[1]] # 一定要转换为向量
# 各国相对于美国的有效制造业劳动力,TABLE 4 的第三列
adjusted_relative_labor <- exp(labor[1:N]) * exp(0.06 * edu_year) /
  (exp(labor[N]) * exp(0.06 * edu_year[N]))
# 各国相对于美国的有效(经人力资本调整)工资
adjusted_relative_wage <- exp(wage[1:N]) * exp(-0.06 * edu_year) /
  (exp(wage[N]) * exp(-0.06 * edu_year[N]))
# 各国相对于美国的人口密度
relative_density <- exp(density[1:N]) / exp(density[N])


table4 <- data.table(
  country = country_table$name,
  research_stock = relative_r_and_d %>% sprintf("%.4f", .),
  years_of_schooling = edu_year %>% sprintf("%.2f", .),
  labor_force_HK_adjusted = adjusted_relative_labor %>% sprintf("%.3f", .),
  density = relative_density %>% sprintf("%.2f", .)
)

table4 %>%
  set_colnames(c(
    "Country", "Research \\\n Stock \\\n (U.S.=1)", "Years of\\\n Schooling \\\n (years/person)", "Labor Force \\\n (HK adjusted) \\\n (U.S.=1)", "Density \\\n (pop/area) \\\n (U.S.=1)"
  )) %>%
  prettify(caption = "TABLE IV \\\n Data for Alternative Parameters") %>%
  footnote(
    general = "Research stocks, in 1990, are from Coe and Helpman (1995). Average years of schooling $H_i$, in 1985, are from Kyriacou (1991). Labor forces, in 1990, are from Summers and Heston (1991). They are adjusted for human capital by multiplying the country $i$ figure by $e^{0.06H_i}$. See the Appendix for complete definitions.",
    general_title = "\n Note: ",
    footnote_as_chunk = T
  )
TABLE IV
Data for Alternative Parameters
Country Research
Stock
(U.S.=1)
Years of
Schooling
(years/person)
Labor Force
(HK adjusted)
(U.S.=1)
Density
(pop/area)
(U.S.=1)
Australia 0.0087 8.72 0.054 0.08
Austria 0.0063 8.57 0.024 3.43
Belgium 0.0151 9.35 0.029 12.03
Canada 0.0300 9.98 0.095 0.10
Denmark 0.0051 6.91 0.017 4.47
Finland 0.0053 10.83 0.019 0.55
France 0.1108 9.54 0.181 3.88
Germany 0.1683 10.33 0.225 9.50
Greece 0.0005 8.40 0.025 2.87
Italy 0.0446 9.13 0.159 7.16
Japan 0.2493 9.47 0.544 12.42
Netherlands 0.0278 9.47 0.043 13.64
New Zealand 0.0010 9.27 0.010 0.47
Norway 0.0057 9.24 0.015 0.49
Portugal 0.0007 6.52 0.026 4.01
Spain 0.0084 9.70 0.100 2.88
Sweden 0.0207 9.64 0.031 0.71
United Kingdom 0.1423 8.50 0.186 8.76
United States 1.0000 12.09 1.000 1.00

Note:
Research stocks, in 1990, are from Coe and Helpman (1995). Average years of schooling \(H_i\), in 1985, are from Kyriacou (1991). Labor forces, in 1990, are from Summers and Heston (1991). They are adjusted for human capital by multiplying the country \(i\) figure by \(e^{0.06H_i}\). See the Appendix for complete definitions.

TABLE V

估计 Section 5.2 的未编号公式

source_parameters <- gls_estimate[11:29]

OLS estimation

competitiveness <- data.table(
  research_stock = log(relative_r_and_d),
  human_capital = 1 / edu_year,
  wage = log(adjusted_relative_wage)
) %>%
  cbind(source_parameters, .)

lm_table5 <- lm(source_parameters ~ ., data = competitiveness)
summary(lm_table5)
#> 
#> Call:
#> lm(formula = source_parameters ~ ., data = competitiveness)
#> 
#> Residuals:
#>      Min       1Q   Median       3Q      Max 
#> -2.63550 -0.31749  0.09465  0.59003  1.46797 
#> 
#> Coefficients:
#>                Estimate Std. Error t value Pr(>|t|)    
#> (Intercept)      5.8130     2.0655   2.814   0.0131 *  
#> research_stock   1.0384     0.1728   6.010 2.39e-05 ***
#> human_capital  -18.0562    20.5483  -0.879   0.3934    
#> wage            -2.8472     1.0227  -2.784   0.0139 *  
#> ---
#> Signif. codes:  0 '***' 0.001 '**' 0.01 '*' 0.05 '.' 0.1 ' ' 1
#> 
#> Residual standard error: 1.109 on 15 degrees of freedom
#> Multiple R-squared:  0.7703, Adjusted R-squared:  0.7244 
#> F-statistic: 16.77 on 3 and 15 DF,  p-value: 4.673e-05

IV estimation

工资与技术水平之间可能存在内生性问题

将劳动力和人口密度作为工资的工具变量,这二者外生于技术

relative_density <- exp(density[1:N]) / exp(density[N])

competitiveness_2SLS <- data.table(
  research_stock = log(relative_r_and_d),
  human_capital = 1 / edu_year,
  wage = log(adjusted_relative_wage),
  labor = log(adjusted_relative_labor),
  density = log(relative_density)
) %>%
  cbind(source_parameters, .)

fit_iv <- ivreg(
  formula = source_parameters ~ research_stock + human_capital + wage |
    research_stock + human_capital + labor + density,
  data = competitiveness_2SLS
)
summary(fit_iv, test = TRUE)
#> 
#> Call:
#> ivreg(formula = source_parameters ~ research_stock + human_capital + 
#>     wage | research_stock + human_capital + labor + density, 
#>     data = competitiveness_2SLS)
#> 
#> Residuals:
#>     Min      1Q  Median      3Q     Max 
#> -2.4724 -0.5927  0.0668  0.6626  1.3383 
#> 
#> Coefficients:
#>                Estimate Std. Error t value Pr(>|t|)    
#> (Intercept)      6.4385     2.1624   2.978  0.00939 ** 
#> research_stock   1.0941     0.1815   6.027 2.32e-05 ***
#> human_capital  -22.6873    21.2475  -1.068  0.30251    
#> wage            -3.5988     1.2054  -2.986  0.00924 ** 
#> 
#> Diagnostic tests:
#>                  df1 df2 statistic  p-value    
#> Weak instruments   2  14    20.538 6.86e-05 ***
#> Wu-Hausman         1  14     1.654   0.2193    
#> Sargan             1  NA     3.229   0.0723 .  
#> ---
#> Signif. codes:  0 '***' 0.001 '**' 0.01 '*' 0.05 '.' 0.1 ' ' 1
#> 
#> Residual standard error: 1.129 on 15 degrees of freedom
#> Multiple R-Squared: 0.7621,  Adjusted R-squared: 0.7145 
#> Wald test: 16.67 on 3 and 15 DF,  p-value: 4.843e-05

估计得 \(\theta=3.60(1.21)\)

Section 5.4

TABLE VI

由 (30) 式估计的 \(S\) 和各种方法估计的 \(\theta\),利用 (27) 式计算技术水平 \(T\)(另一种思路是由 Section 5.2 估计的 \(a_0\)\(a_R\)\(a_H\) 计算 \(T\)

table6 <- theta_estimates %>%
  map_dfc(function(theta) {
    # (27) 式变形
    tech <- log(adjusted_relative_wage) %>% # ln(w_i)
      `*`(theta) %>% # * theta
      `+`(source_parameters) %>% # + S_i
      `*`(beta) %>% # × beta
      exp() # e^

    (tech / tech[N]) %>%
      sprintf("%.2f", .) %>%
      as.data.frame() %>%
      set_colnames(str_c("$\\theta=", sprintf("%.2f", theta), "$"))
  }) %>%
  mutate(
    Country = country_table$name,
    `Estimated Source-country Competitiveness` = source_parameters %>% sprintf("%.2f", .)
  ) %>%
  select(Country, `Estimated Source-country Competitiveness`, everything())


table6 %>%
  prettify(caption = "TABLE VI \\\n States of Technology") %>%
  footnote(
    general = "The estimates of source-country competitiveness are the same as those shown in Table III. For an estimated parameter $\\hat{S_i}$, the implied state of technology is $T_i=(e^{\\hat{S_i}}w_i^\\theta)^\\beta$. States of technology are normalized relative to the U.S. value.",
    general_title = "\n Note: ",
    footnote_as_chunk = T
  ) %>%
  add_header_above(c(
    " " = 1, " " = 1,
    "Implied States of Technology" = 3
  ))
TABLE VI
States of Technology
Implied States of Technology
Country Estimated Source-country Competitiveness \(\theta=3.60\) \(\theta=8.28\) \(\theta=12.86\)
Australia 0.19 0.36 0.27 0.20
Austria -1.16 0.30 0.26 0.23
Belgium -3.34 0.22 0.24 0.26
Canada 0.41 0.47 0.46 0.46
Denmark -1.75 0.32 0.35 0.38
Finland -0.52 0.41 0.45 0.50
France 1.28 0.60 0.64 0.69
Germany 2.35 0.75 0.81 0.86
Greece -2.81 0.14 0.07 0.04
Italy 1.78 0.57 0.50 0.45
Japan 4.20 0.97 0.89 0.81
Netherlands -2.19 0.28 0.30 0.32
New Zealand -1.20 0.22 0.12 0.07
Norway -1.35 0.37 0.43 0.50
Portugal -1.57 0.13 0.04 0.01
Spain 0.30 0.33 0.21 0.14
Sweden 0.01 0.47 0.51 0.57
United Kingdom 1.37 0.53 0.49 0.44
United States 3.98 1.00 1.00 1.00

Note:
The estimates of source-country competitiveness are the same as those shown in Table III. For an estimated parameter \(\hat{S_i}\), the implied state of technology is \(T_i=(e^{\hat{S_i}}w_i^\theta)^\beta\). States of technology are normalized relative to the U.S. value.

TABLE VII

用 (29) 式计算贸易障碍

barrier_parameters <- gls_estimate[-11:-29]

barrier_names <- c(
  "Distance [0, 375)", "Distance [375, 750)", "Distance [750, 1500)",
  "Distance [1500, 3000)", "Distance [3000, 6000)", "Distance [6000, maximum)",
  "Shared border", "Shared language", "Both in EEC/EU", "Both in EFTA",
  country_table$name
)

table7 <- theta_estimates %>%
  map_dfc(function(theta) {
    # (29), (30) 变形
    (barrier_parameters / (-theta)) %>% # 除以 -theta, 才是对 ln(d_ni) 的影响
      exp() %>% # 对dni的影响
      `-`(1) %>%
      `*`(100) %>% # 百分比变化
      sprintf("%.2f", .) %>%
      as.data.frame() %>%
      set_colnames(str_c("$\\theta=", sprintf("%.2f", theta), "$"))
  }) %>%
  mutate(
    source_of_barrier = barrier_names,
    parameters = barrier_parameters %>% sprintf("%.2f", .)
  ) %>%
  select(source_of_barrier, parameters, everything())

table7 %>%
  rename(
    `Source of Barrier` = source_of_barrier,
    `Estimated Geograpy Parameters` = parameters
  ) %>%
  prettify(caption = "TABLE VII \\\n Geographic Barriers") %>%
  footnote(
    general = "The estimated parameters governing geographic barriers are the same as those shown in Table III. For an estimated parameter $\\hat{d}$, the implied effect on cost is $(e^{-\\hat{d}/\\theta}-1) \\times 100\\%$.",
    general_title = "\n Note: ",
    footnote_as_chunk = T
  ) %>%
  add_header_above(c(
    " " = 1, " " = 1,
    "Implied Barrier's $\\%$ Effect on Cost" = 3
  )) %>%
  group_rows("Destination country:", 11, 29,
    bold = FALSE,
    label_row_css = "border-top: 1px solid;"
  )
TABLE VII
Geographic Barriers
Implied Barrier’s \(\%\) Effect on Cost
Source of Barrier Estimated Geograpy Parameters \(\theta=3.60\) \(\theta=8.28\) \(\theta=12.86\)
Distance [0, 375) -3.10 136.51 45.39 27.25
Distance [375, 750) -3.66 176.74 55.67 32.97
Distance [750, 1500) -4.03 206.65 62.77 36.85
Distance [1500, 3000) -4.22 222.75 66.44 38.82
Distance [3000, 6000) -6.06 439.04 108.02 60.25
Distance [6000, maximum) -6.56 518.43 120.82 66.54
Shared border 0.30 -7.89 -3.51 -2.27
Shared language 0.51 -13.25 -5.99 -3.90
Both in EEC/EU 0.04 -1.02 -0.44 -0.29
Both in EFTA 0.54 -13.85 -6.28 -4.09
Destination country:
Australia 0.24 -6.35 -2.81 -1.82
Austria -1.68 59.37 22.46 13.94
Belgium 1.12 -26.74 -12.65 -8.34
Canada 0.69 -17.42 -7.99 -5.22
Denmark -0.51 15.15 6.33 4.03
Finland -1.33 44.88 17.49 10.94
France 0.22 -5.90 -2.61 -1.69
Germany 1.00 -24.27 -11.39 -7.49
Greece -2.36 92.45 32.93 20.11
Italy 0.07 -1.97 -0.86 -0.56
Japan 1.59 -35.62 -17.43 -11.60
Netherlands 1.00 -24.33 -11.42 -7.51
New Zealand 0.07 -1.83 -0.80 -0.52
Norway -1.00 32.06 12.85 8.10
Portugal -1.21 39.82 15.69 9.84
Spain -1.16 37.85 14.98 9.40
Sweden -0.02 0.69 0.30 0.19
United Kingdom 0.81 -20.23 -9.36 -6.13
United States 2.46 -49.49 -25.70 -17.40

Note:
The estimated parameters governing geographic barriers are the same as those shown in Table III. For an estimated parameter \(\hat{d}\), the implied effect on cost is \((e^{-\hat{d}/\theta}-1) \times 100\%\).

总结

estimation 部分,通过各种方式估计 \(\theta\),符号一致,数值有大有小。

选择中间的、也是最简单的矩估计值 \(8.28\),用于后面的 simulation


  1. source dummies 是 (28) 式 \(S_i-S_n\) 的形式。↩︎

  2. 这并非 (28) 式,它用 \(D_{ni}\) 替代了 \(\ln d_{ni}\),还添加了进口国虚拟变量。事实上,EK 的源代码从未估计过 (28) 式。↩︎

  3. 朱建平, 胡朝霞, 王艺明. 高级计量经济学导论[M]. 北京: 北京大学出版社, 2009: 120-121.↩︎

---
title: "EK2002: Estimation \n"
subtitle: ''
author: "Humoon"
date: "`r Sys.Date()`"
output: html_document
documentclass: ctexart
classoption: hyperref,
---

```{r setup, include = FALSE}
source("../config/Rmarkdown_config.R")

## global options ===================================
knitr::opts_chunk$set(
  width = config$width,
  fig.width = config$fig.width,
  fig.asp = config$fig.asp,
  out.width = config$out.width,
  fig.align = config$fig.align,
  fig.path = config$fig.path,
  fig.show = config$fig.show,
  warn = config$warn,
  warning = config$warning,
  message = config$message,
  echo = config$echo,
  eval = config$eval,
  tidy = config$tidy,
  comment = config$comment,
  collapse = config$collapse,
  cache = config$cache,
  cache.comments = config$cache.comments,
  autodep = config$autodep
)
```

```{r, echo=FALSE}
downloadthis::download_dir(
  path = "../data",
  output_name = "data",
  button_label = "Download data dir",
  button_type = "success",
  self_contained = FALSE
)
# downloadthis::download_file(
#   path = "../config/Rmarkdown_config.R",
#   output_name = "Rmarkdown_config",
#   button_label = "Download Rmarkdown_config.R",
#   button_type = "success",
#   self_contained = FALSE
# )
```

```{r}
source("../config/Rmarkdown_config.R") # 依赖包的导入和一系列 Rmarkdown 设置
```

## Data Processing

### 数据精度问题

EK2002 作者使用的编程软件是 GAUSS，其数据文件大都是二进制的，无法用文本编辑器打开，只能用 GAUSS 打印到屏幕上，然后手动复制粘贴到文本文件中，以获得本项目的数据源。

然而，图形化界面的 GAUSS IDE，只能显示小数点后三位，这意味着手动复制粘贴的数据从一开始就是不精确的，会影响所有结果的精度。

只有在命令行风格的 GAUSS Terminal Interface 中打印，才能显示数据的完整位数。从这里复制粘贴，才能保证本项目中数据的精确度。

### Read Data

```{r}
# 一些标量常数
scalar <- jsonlite::fromJSON("../data/scalar.json")

# 国家代码表
country_table <- fread("../data/country_code.csv")

# 用于参数估计的数据，数值型变量大多经过了对数标准化
regression_data <- fread("../data/regression_data.csv")

# 19国50产业价格数据
price_table <- fread("../data/price.csv")
```

看一下数据结构：

```{r}
country_table %>% prettify()
regression_data
price_table
```

### Data Transforming


```{r}
## scalar.json

N <- scalar$N # 国家数量
beta <- scalar$beta # 各国平均 beta
theta_estimates <- scalar$theta # 三种不同水平的theta值
```

```{r}
## regression_data.csv

# 进出口国 index
c(import_country, export_country) %<-% regression_data[, c(1, 2)]


# 对数标准化的制造业双边贸易数据 ln(Xni/Xnn)
trade <- regression_data[, 4] %>% pull()

# ln(X'ni/X'nn), (26)式等号的左边
trade_prime <- regression_data[, 5] %>% pull()

# 由ln(X'ni)的定义可计算(12)式的左边 ln (Xni/Xn)/(Xii/Xi)
# 可将其视为 country n's normalized import share from country i
normalized_trade_share <- -(trade_prime - trade) * beta / (1 - beta) + trade


# 六档距离，说明见P21
c(dist1, dist2, dist3, dist4, dist5, dist6) %<-% regression_data[, 6:11]

# 是否share border/language, 是否均在 EEC/EFTA 中
# 欧共体EEC是EU的前身，EFTA是欧自联
c(border, language, EU, EFTA) %<-% regression_data[, c(12, 18, 19, 20)]

# 横向合并distance, border, language, RTA 等虚拟变量
# 注意，六档距离只需要5个dummy variable
geography_dummy <- cbind(dist2, dist3, dist4, dist5, dist6, border, language, EU, EFTA)


# 以下5个变量的数值都是对数标准化的，即 ln(var_i/var_n)
# 分别是(1)R&D 支出, (2)以平均受教育年限来衡量的 human capital
# (3)人口密度, (4)制造业劳动力数量, (5)工资（均以美元计）
c(r_and_d, human_capital, density, labor, wage) %<-% regression_data[, 13:17]


# 国家首都之间的距离
distance <- regression_data$distance
ln_distance <- log(distance) # 化为对数距离


# 进口国（目的地国）虚拟变量的稀疏矩阵
destination_matrix <- kronecker(diag(N), rep(1, N)) # 克罗内克积
destination_matrix %>%
  as.data.table() %>%
  set_colnames(1:19 %>% str_c("m", .))
# 出口国（来源国）虚拟变量的稀疏矩阵
source_matrix <- kronecker(rep(1, N), diag(N))
source_matrix %>%
  as.data.table() %>%
  set_colnames(1:19 %>% str_c("S", .))

# 来源国虚拟变量 S_i-S_n, (28)式
source_dummy <- source_matrix - destination_matrix
# 这个减法决定了 source_dummy 和 destination_dummy 在(30)式中是不对称的
source_dummy %>% as.data.table() # 观察一下全貌

# 目的地国虚拟变量 m_n, (29)式
destination_dummy <- destination_matrix

# 虚拟变量多一个自由度，要以其中一个为基准
# 用其他虚拟变量与这个基准的相对差异，作为回归模型的自变量
# 以美国（第19列）为基准，前18列都减去19列
relative_source_dummy <- (source_dummy[, -N] - source_dummy[, N]) %>%
  as.data.table() %>% # 矩阵转换为DT
  set_colnames(1:18 %>% str_c("S", .))
relative_source_dummy # 观察一下全貌

relative_destination_dummy <- (destination_dummy[, -N] - destination_dummy[, N]) %>%
  as.data.table() %>%
  set_colnames(1:18 %>% str_c("m", .))
relative_destination_dummy # 观察一下全貌
```


```{r}
## price.csv

# 50种商品的对数标准化价格（以美国为基准）
price <- price_table %>%
  select(-country) %>%
  as.matrix()


# 目的地国50种商品对数标准化价格 ln p_n(j)
destination_price <- kronecker(price, rep(1, N))
# 来源地国50种商品对数标准化价格 ln p_i(j)
source_price <- kronecker(rep(1, N), price)
# r_{ni}(j)=ln p_n(j)-ln p_i(j)
relative_price <- destination_price - source_price
# 各行最大的r_{ni}(j)
max_price <- apply(relative_price, 1, max)
# 各行最大r_{ni}(j)的j（商品种类index）
max_price_index <- apply(relative_price, 1, which.max)
# 遍历各行，将最大的r_{ni}(j)替换为-100
for (k in 1:nrow(relative_price)) {
  relative_price[k, max_price_index[k]] <- -100
}
# 然后求各行第二大的r_{ni}(j)，作为作为ln d_{ni}的代理变量
ln_dni <- max_price2 <- apply(relative_price, 1, max)


# 价格指数
# 用50种商品对数标准化价格的平均值作为各国价格指数的代理变量
mean_price <- apply(price, 1, mean)
# 目的地国价格指数 ln p_n
destination_price_index <- kronecker(mean_price, rep(1, N))
# 来源地国价格指数 ln p_i
source_price_index <- kronecker(rep(1, N), mean_price)
# (13)式: D_{ni}=ln(p_i)-ln(p_n)+ln(d_{ni})
Dni <- source_price_index - destination_price_index + ln_dni
```

```{r}
## delete invalid observations

# 删掉 n==i 的行，保留342行
# 因为这些行自变量和因变量的标准化值都等于0，属于无效数据

# 无效行的index
invalid_line_index <- which(import_country == export_country)

# destinations and sources index
import_country_valid <- import_country[-invalid_line_index]
export_country_valid <- export_country[-invalid_line_index]

# ln (Xni/Xn)/(Xii/Xi)
normalized_trade_share_valid <- normalized_trade_share[-invalid_line_index]

# ln(X'ni/X'nn)
trade_prime_valid <- trade_prime[-invalid_line_index]

# D_{ni}
Dni_valid <- Dni[-invalid_line_index]

# exp(D_{ni})，用于 Figure 2
price_measure <- exp(Dni_valid)

# ln_distance
ln_distance_valid <- ln_distance[-invalid_line_index]

# 合并距离、边界、语言、RTA等虚拟变量
geography_dummy_valid <- geography_dummy[-invalid_line_index, ]

# destinations and sources dummies 组合为数据框
relative_source_dummy_valid <- relative_source_dummy[-invalid_line_index, ]
relative_dest_dummy_valid <- relative_destination_dummy[-invalid_line_index, ]

country_dummy_valid <- cbind(
  relative_dest_dummy_valid,
  relative_source_dummy_valid
) %>% as.data.table()
```

## Section 3

### FIGURE I

```{r, echo=FALSE}
title1 <- "<b>FIGURE I: Trade and Geography</b>"
xtitle1 <- TeX("\\text{distance (in miles) between countries n and i}")
ytitle1 <- TeX("\\text{normalized import share: } \\frac{X_{ni}/Xn}{X_{ii}/X_i}")

fig1 <- canvas %>%
  add_markers(
    x = distance[-invalid_line_index] * 1000, # 单位：mile
    y = exp(normalized_trade_share_valid),
    marker = list(color = "black")
  ) %>%
  academic_layout() %>%
  layout(
    title = list(text = title1),
    xaxis = list(
      type = "log", range = c(2, 5),
      nticks = 4, title = list(text = xtitle1)
    ),
    yaxis = list(
      type = "log", range = c(-4, 0),
      nticks = 5, title = list(text = ytitle1)
    )
  )
fig1
saveWidget(fig1, "../export/Figure1.html",
  selfcontained = F, libdir = "lib"
)
```

```{r}
# 标准化贸易份额的最大值
exp(normalized_trade_share_valid) %>% max()
# 横跨近四个数量级
exp(normalized_trade_share_valid) %>%
  max() %>%
  `/`(exp(normalized_trade_share_valid) %>% min()) %>%
  log() %>%
  `/`(log(10))
```

### FIGURE II

```{r, echo=FALSE}
title2 <- "<b>FIGURE II: Trade and Prices</b>"
xtitle2 <- TeX("\\text{price mearsure: }D_{ni}")
ytitle2 <- TeX("\\text{log of normalized import share: }\\ln \\frac{X_{ni}/Xn}{X_{ii}/X_i}")

fig2 <- canvas %>%
  add_markers(
    x = Dni_valid, y = normalized_trade_share_valid,
    showlegend = FALSE, marker = list(color = "black"),
    opacity = 0.8
  ) %>%
  academic_layout() %>%
  layout(
    title = list(text = title2),
    xaxis = list(range = c(0, 1.4), title = list(text = xtitle2)),
    yaxis = list(range = c(-12, 0), title = list(text = ytitle2))
  )

fig2
saveWidget(fig2, "../export/Figure2.html",
  selfcontained = F, libdir = "lib"
)
```

```{r}
# 相关系数 correlation
cor(Dni_valid, normalized_trade_share_valid)
```

### TABLE II

```{r}
price_measure_table <- # 三列：进口国index，出口国index，exp(Dni)
  cbind(import_country_valid, export_country_valid, price_measure) %>%
  as.data.table() %>% # 转换数据类型
  # 左连接匹配国家代码（code列）
  left_join(country_table, by = c("import_country_valid" = "id")) %>%
  rename(dest = code) %>%
  left_join(country_table, by = c("export_country_valid" = "id")) %>%
  rename(source = code) %>%
  # 挑选这三列，其余删掉
  select(dest, source, price_measure)

price_measure_table


table2 <- country_table$code %>% # 迭代对象: 19个国家代码
  map_dfr( # 每轮迭代生成一行，最后把这些行纵向摞起来
    function(country_code) {

      # select 进口国为country_code的所有的行
      dest_table <- price_measure_table[dest == country_code, ]

      source_min <- dest_table[
        which.min(price_measure), # select price_measure 最小值所在的行
      ][
        , concatenation := str_c(source, "(", sprintf("%0.2f", price_measure), ")")
      ] %>% pull(concatenation)

      source_max <- dest_table[
        which.max(price_measure),
      ][
        , concatenation := str_c(source, "(", sprintf("%0.2f", price_measure), ")")
      ] %>% pull(concatenation)


      # 出口国为country_code的所有的行
      source_table <- price_measure_table[source == country_code, ]

      dest_min <- source_table[
        which.min(price_measure),
      ][
        , concatenation := str_c(dest, "(", sprintf("%0.2f", price_measure), ")")
      ] %>% pull(concatenation)

      dest_max <- source_table[
        which.max(price_measure),
      ][
        , concatenation := str_c(dest, "(", sprintf("%0.2f", price_measure), ")")
      ] %>% pull(concatenation)


      # map_dfr()的每个返回值都是Table II的一行
      data.table(
        Country = str_c(
          country_table[code == country_code, ] %>% pull(name),
          " (", country_code, ")"
        ),
        source_min, source_max, dest_min, dest_max
      )
    }
  )

table2 %>%
  set_colnames(c("Country", "Minimum", "Maximum", "Minimum", "Maximum")) %>%
  prettify(caption = "TABLE II \\\n Price Measure Statistics") %>%
  add_header_above(c(" " = 1, "Foreign Source \n (Column 1 As Destination)" = 2, "Foreign Destinations \n (Column 1 As Source)" = 2)) %>%
  footnote(
    general = "本表中的数值为 $e^{D_{ni}}$，其中 $D_{ni}$ 在 (13) 式中定义，为 $\\ln (p_i d_{ni}/p_n)$ 的代理变量。因此，$e^{D_{ni}}$ 表示进口国 $n$ 若全部从出口国 $i$ 的市场购买商品（花费当地价格及运输成本），比实际的购买（在本国市场充分遵循比较优势）会贵多少。",
    general_title = "\n Note: ",
    footnote_as_chunk = T
  )
```

### 用 (12) 式估计 $\theta$

以 $\ln (Xni/Xn)/(Xii/Xi)$ 为被解释变量，以 $D_{ni}$ 为解释变量，估计出来的系数是 $-\theta$，因此 $\theta$ 值还要取一个负号。

#### Moments Estimation

最简单的一阶矩估计

```{r}
x_center <- mean(Dni_valid)
y_center <- mean(normalized_trade_share_valid)
theta <- y_center / x_center
theta
```

$\theta=8.28$

#### OLS Estimation

```{r}
# 无截距项
lm_1 <- lm(normalized_trade_share_valid ~ 0 + Dni_valid)
summary(lm_1) %>%
  `[[`("coefficients") %>%
  prettify()
```

$\theta=8.03(0.15)$, 与矩估计的估计值很接近。

```{r}
# 有截距项
lm_2 <- lm(normalized_trade_share_valid ~ Dni_valid)
summary(lm_2) %>%
  `[[`("coefficients") %>%
  prettify()
```

$\theta=4.57(0.56)$. 截距项为负，与理论预测（为0）不一致，表明数据中可能有较大的误差.

```{r, echo=FALSE}
xs <- data.table(Dni_valid = Dni_valid)
ys_hat1 <- fitted(lm_1)
ys_hat2 <- fitted(lm_2)

# 绘图
title2 <- "<b>FIGURE 2: Trade and Prices</b>"
xtitle2 <- TeX("\\text{price mearsure: }D_{ni}")
ytitle2 <- TeX("\\text{log of normalized import share: }\\ln \\frac{X_{ni}/Xn}{X_{ii}/X_i}")

fig2 %>%
  add_lines(
    line = list(color = "royalblue"),
    x = xs$Dni_valid, y = ys_hat1, name = "no constant<br>OLS estimation",
    opacity = 0.8
  ) %>%
  add_lines(
    line = list(color = "green"),
    x = xs$Dni_valid, y = ys_hat2, name = "with constant<br>OLS estimation",
    opacity = 0.8
  ) %>%
  add_markers(
    x = x_center, y = y_center, name = "moments estimation",
    marker = list(color = "red", size = 10)
  ) %>%
  add_lines(
    line = list(color = "orangered", dash = "dot"),
    x = c(0, x_center), y = c(0, y_center), showlegend = FALSE
  )
```

#### 分别估计 $D_{ni}$ 三个组成部分的参数

探讨 $D_{ni}$ 三个组成部分 $\ln p_i, \ln p_n, \ln d_{ni}$ 对标准化贸易份额的分别贡献。

```{r}
# 三个组成部分分别为三列，去掉无效行
trade_share_components <- data.table(
  y = normalized_trade_share_valid,
  ln_pi = source_price_index[-invalid_line_index],
  ln_pn = destination_price_index[-invalid_line_index],
  ln_dni = ln_dni[-invalid_line_index]
)

# 无截距项
lm_3 <- lm(y ~ 0 + ln_pi + ln_pn + ln_dni, data = trade_share_components)
summary(lm_3) %>%
  `[[`("coefficients") %>%
  prettify()

# 有截距项
lm_4 <- lm(y ~ ln_pi + ln_pn + ln_dni, data = trade_share_components)
summary(lm_4) %>%
  `[[`("coefficients") %>%
  prettify()
```

无论有无截距项，估计出来的参数的正负与理论预测的一致

#### IV Estimation

有截距 OLS 回归的截距不为0，表明我们的价格数据可能有系统误差。

为 price measure $D_{ni}$ 寻找工具变量（IV），用工具变量法估计 $\theta$ ([**以下两种估计仅在源代码中出现，未在论文中出现**]{style="color:red"}).

1. 以对数实际距离作为 $D_{ni}$ 的工具变量

```{r, echo=FALSE}
# # 第一阶段：D_{ni} 对工具变量 ln_distance 做回归
# lm_6 <- lm(Dni_valid ~ ln_distance_valid)
# Dni_fitted <- fitted(lm_6) # Dni^hat

# # 第二阶段：对数标准化贸易份额再对 Dni^hat 回归
# lm_7 <- lm(normalized_trade_share_valid ~ Dni_fitted)
# summary(lm_7)
```

```{r}
# ivreg::ivreg() 可以做工具变量回归，第一个参数（字符串）为回归公式，形式为：
# 被解释变量 ~ 内生变量 + 外生变量 | 工具变量 + 外生变量
fit_iv_1 <- ivreg(normalized_trade_share_valid ~ Dni_valid | ln_distance_valid)
summary(fit_iv_1, test = TRUE) # 对IV回归进行诊断
```

IV 回归通过了诊断，$\theta=14.51(1.57)$

2. 以地理距离、source[^3] & destination dummies 作为 $D_{ni}$ 的工具变量

[^3]: source dummies 是 (28) 式 $S_i-S_n$ 的形式。

```{r, echo=FALSE}
# 2SLS 实现 IV estimation

# lm_8 <- lm(Dni_valid ~ .,
#   data = cbind(Dni_valid, ln_distance_valid, country_dummy_valid)
# )
# Dni_fitted <- fitted(lm_8) # Dni^hat
# lm_9 <- lm(normalized_trade_share_valid ~ Dni_fitted)
# summary(lm_9)
```

```{r}
instrument_data <- cbind(ln_distance_valid, country_dummy_valid)
formula_instrument <- colnames(instrument_data) %>% str_c(collapse = " + ")
formula_instrument

fit_iv_2 <- ivreg(
  formula = str_c("normalized_trade_share_valid ~ Dni_valid | ", formula_instrument),
  data = cbind(normalized_trade_share_valid, Dni_valid, instrument_data)
)
summary(fit_iv_2, test = TRUE)
```

$\theta=6.90(0.71)$


## Section 5.3

估计一个结果被报告在正文中、但方程从未出现过的计量模型[^4]：以 $\ln (X'_{ni}/X'_{nn})$ 为被解释变量，$D_{ni}$ 为内生解释变量，source & destination dummies 为外生解释变量

[^4]: 这并非 (28) 式，它用 $D_{ni}$ 替代了 $\ln d_{ni}$，还添加了进口国虚拟变量。事实上，EK 的源代码从未估计过 (28) 式。

### OLS Estimation

```{r}
lm_5 <- lm(
  trade_prime_valid ~ ., # . 代表所有其他变量
  data = cbind(trade_prime_valid, Dni_valid, country_dummy_valid)
)
summary(lm_5) %>%
  `[[`("coefficients") %>%
  prettify()
```

$\theta=2.45(0.49)$

### IV Estimation

以 geography_dummies 为工具变量，包括距离、边界、语言、RTA 等，解释内生变量 D_ni；country_dummies 为外生变量。

```{r, echo=FALSE}
# lm_8 <- lm(Dni_valid ~ .,
#   data = cbind(Dni_valid, geography_dummy_valid, country_dummy_valid)
# )
# summary(lm_8)
# Dni_fitted <- fitted(lm_8)
#
# lm_9 <- lm(trade_prime_valid ~ .,
#            data = cbind(trade_prime_valid, Dni_fitted, country_dummy_valid))
# summary(lm_9)
```

```{r}
TSLS_data <- cbind(trade_prime_valid, Dni_valid, geography_dummy_valid, country_dummy_valid)
TSLS_data

# 外生变量
formula_exogenous <- colnames(country_dummy_valid) %>% str_c(collapse = " + ")
formula_exogenous

# 工具变量
formula_instrument <- colnames(geography_dummy_valid) %>% str_c(collapse = " + ")
formula_instrument

# 回归公式
formula <- str_c(
  "trade_prime_valid ~ Dni_valid + ", formula_exogenous, " | ",
  formula_instrument, " + ", formula_exogenous
)
formula

fit_iv_3 <- ivreg(formula = formula, data = TSLS_data)
summary(fit_iv_3, test = TRUE)
```

$\theta=12.86(1.74)$

## Section 5.1

### TABLE III

估计 (30) 式

#### OLS estimation

```{r}
# 组织数据框
table3_data <- cbind(
  trade_prime, dist1, geography_dummy,
  relative_source_dummy, relative_destination_dummy
) %>%
  as.data.table() %>%
  `[`(-invalid_line_index, )

# OLS
lm_table3 <- lm(trade_prime ~ 0 + ., data = table3_data)
summary(lm_table3)
```

#### GLS estimation

-   由理论推断，(30) 式的回归模型违反了 OLS 的基本假设: $\text{cov}(\varepsilon_j, \varepsilon_k)=E(\varepsilon_{j}\varepsilon_{k})-E(\varepsilon_{j})E(\varepsilon_{k})=E(\varepsilon_{j}\varepsilon_{k}) = 0, \forall j \neq k$.

    -   这是因为，贸易具有互惠性，如果 $i$ 国向 $n$ 国出口的贸易障碍偏低（实际值低于模型拟合值），则一般 $n$ 国向 $i$ 国出口的贸易障碍也会偏低。这两个误差 $\varepsilon_{n \leftarrow i}, \varepsilon_{i\leftarrow n}$（以下简写为 $\varepsilon_{ni}$ 和 $\varepsilon_{in}$）往往同时偏高或偏低，有一定相关性，故 $\text{cov}(\varepsilon_{ni}, \varepsilon_{in})>0$

    -   设误差 $\varepsilon_{ni}=\varepsilon_{ni}^1+\varepsilon_{ni}^2$ 可以分为两部分，**两部分之间不相关**

    -   第一部分 $\varepsilon_{ni}^1$ 符合 OLS 的经典假设，即 $\begin{aligned}E(\varepsilon_{ab}^1\varepsilon_{cd}^1) = \left\{\begin{matrix} \sigma_1^2, & \forall a=c \land b=d\\ 0, & \text{otherwise.} \end{matrix}\right.\end{aligned}$

    -   第二部分专门体现两国贸易的互惠性，有性质 $\varepsilon_{ni}^2=\varepsilon_{in}^2$，使得 $E(\varepsilon_{ni}^2\varepsilon_{in}^2)= E(\varepsilon_{ni}^2\varepsilon_{ni}^2) =\sigma_2^2$

    -   则总误差满足 \begin{align}
        E(\varepsilon_{ab}\varepsilon_{cd}) & = E(\varepsilon_{ab}^1\varepsilon_{cd}^1)+E(\varepsilon_{ab}^1\varepsilon_{cd}^2)+E(\varepsilon_{ab}^2\varepsilon_{cd}^1)+E(\varepsilon_{ab}^2\varepsilon_{cd}^2) \\
        &=E(\varepsilon_{ab}^1\varepsilon_{cd}^1)+E(\varepsilon_{ab}^2\varepsilon_{cd}^2) \\

        &= \left\{\begin{matrix}
        \sigma_1^2+\sigma_2^2, & \forall a=c \land  b=d  \\
         \sigma_2^2, & \forall a=d \land b=c\\
        0, & \text{otherwise.}
        \end{matrix}\right.
        \end{align}

-   误差项有了上述性质，便不能再使用 OLS estimation，而应使用广义最小二乘法（GLS）[^5]。

    -   设误差向量 $\boldsymbol{\varepsilon}$ 的协方差矩阵为 $\boldsymbol{\Omega}$，则系数向量 $\boldsymbol{\beta}$ 在经过一定变换后的新模型中的 GLS estimator 为 $\hat{\boldsymbol{\beta}}^\ast=(\boldsymbol{X}'\boldsymbol{\Omega}^{-1}\boldsymbol{X})^{-1}\boldsymbol{X}'\boldsymbol{\Omega}^{-1}\boldsymbol{Y}$，协方差矩阵为 $\text{Var}(\hat{\boldsymbol{\beta}}^\ast)=(\boldsymbol{X}'\boldsymbol{\Omega}^{-1}\boldsymbol{X})^{-1}$
    -   事实上，$\boldsymbol{\Omega}$ 的具体形式是很难了解的。但在本文中，可以根据理论，使用 $\boldsymbol{e}\boldsymbol{e}'$ 对其进行估计（$\boldsymbol{e}$ 为残差向量）

-   对于纯粹的异方差问题（误差的协方差矩阵只是对角元素不同，但非对角元素保证为 0），R base 中有 `lm()` 或 `lm.gls()` 函数可以直接用；但对于协方差矩阵非对角元素不为零的情况，目前似乎没有很好的 library 提供现成的函数，需要自己写矩阵运算。

[^5]: 朱建平, 胡朝霞, 王艺明. 高级计量经济学导论[M]. 北京: 北京大学出版社, 2009: 120-121.


```{r}
# 由 OLS 求得所有观测的残差，并将其扩展为矩阵，作为估计误差协方差的材料
ee_matrix <- lm_table3$residuals %o% lm_table3$residuals
# 这是一个 342*342 的大矩阵

# 估计 sigma_1^2 + sigma_2^2
sum_sigma_square <- diag(ee_matrix) %>% # 从n到i与从n到i的trade_prime的残差之积
  mean() # 期望为 sigma_1^2 + sigma_2^2

# 估计 sigma_2^2
observation_valid <- data.table(n = import_country, i = export_country) %>%
  `[`(-invalid_line_index, ) %>%
  `[`(, row_index := .I)

print(observation_valid)

sigma2_square <- observation_valid$row_index %>%
  map_dbl(function(row_index) {
    row_n <- observation_valid$n[row_index]
    row_i <- observation_valid$i[row_index]
    col_index <- observation_valid[n == row_i & i == row_n, ]$row_index
    ee_matrix[row_index, col_index] # 从n到i与从i到n的trade_prime的残差之积
  }) %>%
  mean() # 期望为 sigma_2^2

sigma2_square
sum_sigma_square - sigma2_square
```

因此

$\theta^2\sigma_2^2=$ `r round(sigma2_square, 2)`

$\theta^2\sigma_1^2=$ `r round(sum_sigma_square-sigma2_square, 2)`


```{r}
# 误差协方差矩阵 Omega
Omega <- diag(nrow(observation_valid)) * sum_sigma_square

observation_valid$row_index %>%
  walk(function(row_index) {
    row_n <- observation_valid$n[row_index]
    row_i <- observation_valid$i[row_index]
    col_index <- observation_valid[n == row_i & i == row_n, ]$row_index
    Omega[row_index, col_index] <<- sigma2_square # "<<-" 对环境外变量赋值
  })

Omega %>% round(2) %>% as.data.table()

# 求逆
Omega_inverse <- solve(Omega)

# GLS estimation
Y <- table3_data$trade_prime
X <- table3_data[, -1] %>% as.matrix()

estimate <- solve(t(X) %*% Omega_inverse %*% X) %*% t(X) %*% Omega_inverse %*% Y
estimate_S19 <- -estimate[11:28] %>% sum() # 保证虚拟变量效应之和为0
estimate_m19 <- -estimate[29:46] %>% sum()

var_estimate <- solve(t(X) %*% Omega_inverse %*% X)
stand_error <- diag(var_estimate) %>% sqrt()
stand_error_S19 <- var_estimate[11:28, 11:28] %>%
  sum() %>% # -S19等于S1到S18的和，因此S19的方差应等于S1到S18所有的方差和协方差之和
  sqrt()
stand_error_m19 <- var_estimate[29:46, 29:46] %>%
  sum() %>%
  sqrt()
```

```{r}
# Table III
gls_estimate <- c(
  estimate[1:28], estimate_S19,
  estimate[29:46], estimate_m19
)
gls_stand_error <- c(
  stand_error[1:28], stand_error_S19,
  stand_error[29:46], stand_error_m19
)
gls_parameters <- c(
  1:6 %>% str_c("$-\\theta d_{", ., "}$"),
  "$-\\theta b$", "$-\\theta l$", "$-\\theta e_1$", "$-\\theta e_2$",
  1:19 %>% str_c("$S_{", ., "}$"),
  1:19 %>% str_c("$-\\theta m_{", ., "}$")
)
variable_names <- c(
  "Distance [0, 375)", "Distance [375, 750)", "Distance [750, 1500)",
  "Distance [1500, 3000)", "Distance [3000, 6000)", "Distance [6000, maximum)",
  "Shared border", "Shared language", "Both in EEC/EU", "Both in EFTA",
  country_table$name %>% str_c("Source country: ", .),
  country_table$name %>% str_c("Destination country: ", .)
)


table3 <- data.table(
  variables = variable_names,
  parameters = gls_parameters,
  estimate = round(gls_estimate, 2),
  std_error = round(gls_stand_error, 2)
)

table3 %>%
  mutate(std_error = str_c("(", std_error, ")")) %>%
  set_colnames(c("Variable", "parameter", "est.", "s.e.")) %>%
  prettify(caption = "TABLE III \\\n Bilateral Trade Equation") %>%
  footnote(
    general = "Estimated by GLS. The parameter are normalized so that ${\\textstyle \\sum_{i=1}^{19} S_i}=0$ and ${\\textstyle \\sum_{n=1}^{19} m_n}=0$. Standard errors are in parentheses.",
    general_title = "\n Note: ",
    footnote_as_chunk = T
  )
```

#### 保存估计结果

TABLE III 的估计值对于下一步的 simulation 非常重要。

1. Source country dummy 的估计值可用于计算各国技术水平
2. 其他虚拟变量的估计值（$-\theta \ln(d_{ni})$ 各组成部分的系数）可计算 $-\theta \ln(d_{ni})$ 的拟合值。将此拟合值命名为 barrier_measure，作为 simulation 阶段 $d_{ni}$ 的数据来源。

```{r}
table3_estimate <- gls_estimate # 是用高精度估计值
# table3$estimate 的数据只有两位小数，不能用

barrier_dummy <- cbind(regression_data[, c(6:12, 18:20)], destination_dummy) %>%
  as.matrix() # 361*29
barrier_estimate <- gls_estimate[c(1:10, 30:48)] # 29*1

barrier_measure <- barrier_dummy %*% barrier_estimate %>% # 361*1
  `[<-`(invalid_line_index, 0) %>% # n==i 的行取0
  matrix(nrow = N, byrow = TRUE)
```

```{r}
# 保存为 R 二进制文件 .rda，使用时直接 load()
save(table3_estimate, barrier_measure,
  file = "../data/estimation-output.rda"
)
```

## Section 5.2

### TABLE IV

```{r}
# 所有国家相对于美国的 R&D stock，TABLE 4 的第一列
relative_r_and_d <- exp(r_and_d[1:N]) / exp(r_and_d[N])
# 各国平均教育年限，TABLE 4 的第二列
edu_year <- regression_data[1:N, 22][[1]] # 一定要转换为向量
# 各国相对于美国的有效制造业劳动力，TABLE 4 的第三列
adjusted_relative_labor <- exp(labor[1:N]) * exp(0.06 * edu_year) /
  (exp(labor[N]) * exp(0.06 * edu_year[N]))
# 各国相对于美国的有效（经人力资本调整）工资
adjusted_relative_wage <- exp(wage[1:N]) * exp(-0.06 * edu_year) /
  (exp(wage[N]) * exp(-0.06 * edu_year[N]))
# 各国相对于美国的人口密度
relative_density <- exp(density[1:N]) / exp(density[N])


table4 <- data.table(
  country = country_table$name,
  research_stock = relative_r_and_d %>% sprintf("%.4f", .),
  years_of_schooling = edu_year %>% sprintf("%.2f", .),
  labor_force_HK_adjusted = adjusted_relative_labor %>% sprintf("%.3f", .),
  density = relative_density %>% sprintf("%.2f", .)
)

table4 %>%
  set_colnames(c(
    "Country", "Research \\\n Stock \\\n (U.S.=1)", "Years of\\\n Schooling \\\n (years/person)", "Labor Force \\\n (HK adjusted) \\\n (U.S.=1)", "Density \\\n (pop/area) \\\n (U.S.=1)"
  )) %>%
  prettify(caption = "TABLE IV \\\n Data for Alternative Parameters") %>%
  footnote(
    general = "Research stocks, in 1990, are from Coe and Helpman (1995). Average years of schooling $H_i$, in 1985, are from Kyriacou (1991). Labor forces, in 1990, are from Summers and Heston (1991). They are adjusted for human capital by multiplying the country $i$ figure by $e^{0.06H_i}$. See the Appendix for complete definitions.",
    general_title = "\n Note: ",
    footnote_as_chunk = T
  )
```

### TABLE V

估计 Section 5.2 的未编号公式

```{r}
source_parameters <- gls_estimate[11:29]
```

#### OLS estimation

```{r}
competitiveness <- data.table(
  research_stock = log(relative_r_and_d),
  human_capital = 1 / edu_year,
  wage = log(adjusted_relative_wage)
) %>%
  cbind(source_parameters, .)

lm_table5 <- lm(source_parameters ~ ., data = competitiveness)
summary(lm_table5)
```

#### IV estimation

工资与技术水平之间可能存在内生性问题

将劳动力和人口密度作为工资的工具变量，这二者外生于技术

```{r}
relative_density <- exp(density[1:N]) / exp(density[N])

competitiveness_2SLS <- data.table(
  research_stock = log(relative_r_and_d),
  human_capital = 1 / edu_year,
  wage = log(adjusted_relative_wage),
  labor = log(adjusted_relative_labor),
  density = log(relative_density)
) %>%
  cbind(source_parameters, .)

fit_iv <- ivreg(
  formula = source_parameters ~ research_stock + human_capital + wage |
    research_stock + human_capital + labor + density,
  data = competitiveness_2SLS
)
summary(fit_iv, test = TRUE)
```

估计得 $\theta=3.60(1.21)$



## Section 5.4

### TABLE VI

由 (30) 式估计的 $S$ 和各种方法估计的 $\theta$，利用 (27) 式计算技术水平 $T$（另一种思路是由 Section 5.2 估计的 $a_0$、$a_R$、$a_H$ 计算 $T$）

```{r}
table6 <- theta_estimates %>%
  map_dfc(function(theta) {
    # (27) 式变形
    tech <- log(adjusted_relative_wage) %>% # ln(w_i)
      `*`(theta) %>% # * theta
      `+`(source_parameters) %>% # + S_i
      `*`(beta) %>% # × beta
      exp() # e^

    (tech / tech[N]) %>%
      sprintf("%.2f", .) %>%
      as.data.frame() %>%
      set_colnames(str_c("$\\theta=", sprintf("%.2f", theta), "$"))
  }) %>%
  mutate(
    Country = country_table$name,
    `Estimated Source-country Competitiveness` = source_parameters %>% sprintf("%.2f", .)
  ) %>%
  select(Country, `Estimated Source-country Competitiveness`, everything())


table6 %>%
  prettify(caption = "TABLE VI \\\n States of Technology") %>%
  footnote(
    general = "The estimates of source-country competitiveness are the same as those shown in Table III. For an estimated parameter $\\hat{S_i}$, the implied state of technology is $T_i=(e^{\\hat{S_i}}w_i^\\theta)^\\beta$. States of technology are normalized relative to the U.S. value.",
    general_title = "\n Note: ",
    footnote_as_chunk = T
  ) %>%
  add_header_above(c(
    " " = 1, " " = 1,
    "Implied States of Technology" = 3
  ))
```

### TABLE VII

用 (29) 式计算贸易障碍

```{r}
barrier_parameters <- gls_estimate[-11:-29]

barrier_names <- c(
  "Distance [0, 375)", "Distance [375, 750)", "Distance [750, 1500)",
  "Distance [1500, 3000)", "Distance [3000, 6000)", "Distance [6000, maximum)",
  "Shared border", "Shared language", "Both in EEC/EU", "Both in EFTA",
  country_table$name
)

table7 <- theta_estimates %>%
  map_dfc(function(theta) {
    # (29), (30) 变形
    (barrier_parameters / (-theta)) %>% # 除以 -theta, 才是对 ln(d_ni) 的影响
      exp() %>% # 对dni的影响
      `-`(1) %>%
      `*`(100) %>% # 百分比变化
      sprintf("%.2f", .) %>%
      as.data.frame() %>%
      set_colnames(str_c("$\\theta=", sprintf("%.2f", theta), "$"))
  }) %>%
  mutate(
    source_of_barrier = barrier_names,
    parameters = barrier_parameters %>% sprintf("%.2f", .)
  ) %>%
  select(source_of_barrier, parameters, everything())

table7 %>%
  rename(
    `Source of Barrier` = source_of_barrier,
    `Estimated Geograpy Parameters` = parameters
  ) %>%
  prettify(caption = "TABLE VII \\\n Geographic Barriers") %>%
  footnote(
    general = "The estimated parameters governing geographic barriers are the same as those shown in Table III. For an estimated parameter $\\hat{d}$, the implied effect on cost is $(e^{-\\hat{d}/\\theta}-1) \\times 100\\%$.",
    general_title = "\n Note: ",
    footnote_as_chunk = T
  ) %>%
  add_header_above(c(
    " " = 1, " " = 1,
    "Implied Barrier's $\\%$ Effect on Cost" = 3
  )) %>%
  group_rows("Destination country:", 11, 29,
    bold = FALSE,
    label_row_css = "border-top: 1px solid;"
  )
```


## 总结

estimation 部分，通过各种方式估计 $\theta$，符号一致，数值有大有小。

选择中间的、也是最简单的矩估计值 $8.28$，用于后面的 simulation
