地理学报 ›› 2019, Vol. 74 ›› Issue (6): 1131-1148.doi: 10.11821/dlxb201906005
王少剑,黄永源
收稿日期:
2018-04-04
修回日期:
2019-03-11
出版日期:
2019-06-25
发布日期:
2019-06-20
作者简介:
王少剑(1986-), 男, 河南驻马店人, 博士, 副教授, 中国地理学会会员(S110011019M), 研究方向为城市地理、城市与区域规划。E-mail: 1987wangshaojian@163.com
基金资助:
WANG Shaojian,HUANG Yongyuan
Received:
2018-04-04
Revised:
2019-03-11
Published:
2019-06-25
Online:
2019-06-20
Supported by:
摘要:
采用核密度估计、空间自相关、空间马尔科夫链和面板分位数回归等方法对1992-2013年全国283个城市碳排放强度的空间溢出效应和驱动因素进行了分析。① 核密度估计结果表明,中国城市碳排放强度总体均值下降,差异在逐步缩小。② 空间自相关Moran's I指数表明城市碳排放强度存在显著的空间集聚性且空间集聚性在逐渐增强,但空间集聚水平的变化逐年缩小。③ 空间马尔科夫链分析结果表明:第一,中国城市碳排放强度存在马太效应,低强度与高强度的城市在相邻年份转移过程中呈现维持初始状态的特征。第二,城市碳排放“空间溢出”效应明显,且不同区域背景下溢出效应存在异质性,即若与碳排放强度低的城市为邻,该城市的碳强度能够增加向上转移的概率,反之亦然。④ 面板分位数结果显示:在碳排放强度低的城市,经济增长、技术进步、适当的人口密度起到减排作用;外商投资强度与交通排放是使碳强度增大的主要因素。在碳排放强度高的城市,人口密度是重要的减排因素,技术进步暂时没起减排作用;工业排放、粗放式的资本投资以及城市土地蔓延则是碳强度上升的主要因素。
王少剑,黄永源. 中国城市碳排放强度的空间溢出效应及驱动因素[J]. 地理学报, 2019, 74(6): 1131-1148.
WANG Shaojian,HUANG Yongyuan. Spatial spillover effect and driving forces of carbon emission intensity at city level in China[J]. Acta Geographica Sinica, 2019, 74(6): 1131-1148.
表2
中国城市碳排放强度Moran's I指数值
年份 | Moran's I | Z值 | 年份 | Moran's I | Z值 |
---|---|---|---|---|---|
1992 | 0.359 | 8.717** | 2003 | 0.434 | 11.018** |
1993 | 0.416 | 10.459** | 2004 | 0.435 | 10.942** |
1994 | 0.336 | 8.807** | 2005 | 0.498 | 12.424** |
1995 | 0.325 | 8.653** | 2006 | 0.478 | 11.903** |
1996 | 0.292 | 7.565** | 2007 | 0.464 | 11.564** |
1997 | 0.460 | 11.741** | 2008 | 0.443 | 11.003** |
1998 | 0.316 | 8.143** | 2009 | 0.489 | 12.150** |
1999 | 0.431 | 11.005** | 2010 | 0.448 | 11.124** |
2000 | 0.411 | 10.504** | 2011 | 0.435 | 10.880** |
2001 | 0.414 | 10.453** | 2012 | 0.428 | 10.599** |
2002 | 0.417 | 10.516** | 2013 | 0.380 | 9.534** |
表4
1992-2013年中国城市碳排放强度类型空间马尔科夫转移概率矩阵
邻域类型 | t/t+1 | n | 1 | 2 | 3 | 4 |
---|---|---|---|---|---|---|
1 | 1 | 659 | 0.9408 | 0.0561 | 0.0030 | 0 |
2 | 357 | 0.1345 | 0.7703 | 0.0924 | 0.0028 | |
3 | 257 | 0.0039 | 0.2257 | 0.7237 | 0.0467 | |
4 | 176 | 0 | 0 | 0.1364 | 0.8636 | |
2 | 1 | 478 | 0.8766 | 0.1192 | 0.0042 | 0 |
2 | 467 | 0.1370 | 0.7687 | 0.0878 | 0.0064 | |
3 | 314 | 0 | 0.2070 | 0.7516 | 0.0414 | |
4 | 204 | 0.0098 | 0.0049 | 0.1422 | 0.8431 | |
3 | 1 | 244 | 0.8361 | 0.1516 | 0.0123 | 0 |
2 | 462 | 0.1364 | 0.7727 | 0.0887 | 0.0022 | |
3 | 483 | 0.0021 | 0.1843 | 0.7723 | 0.0414 | |
4 | 313 | 0.0032 | 0 | 0.1374 | 0.8594 | |
4 | 1 | 58 | 0.8103 | 0.1724 | 0.0172 | 0 |
2 | 171 | 0.0760 | 0.7778 | 0.1404 | 0.0058 | |
3 | 458 | 0 | 0.1026 | 0.8384 | 0.0590 | |
4 | 842 | 0 | 0 | 0.0855 | 0.9145 |
表5
FE与分位数回归估计结果
变量 | (1) | (2) | (3) | (4) | (5) | (6) |
---|---|---|---|---|---|---|
FE | q10 | q25 | q50 | q75 | q90 | |
A | 2.138*** | 1.5515*** | 1.6227*** | 1.6329*** | 1.4469*** | 1.2669*** |
(8.85) | (4.97) | (5.58) | (5.97) | (5.16) | (5.08) | |
SA | -0.140*** | -0.1018*** | -0.1066*** | -0.1102*** | -0.1071*** | -0.1023*** |
(-10.60) | (-5.69) | (-6.14) | (-6.49) | (-6.15) | (-7.07) | |
P | -0.210*** | -0.0665** | -0.0747*** | -0.0792*** | -0.0813*** | -0.0771*** |
(-2.76) | (-2.42) | (-2.65) | (-2.89) | (-2.97) | (-2.81) | |
IS | 0.369*** | 0.1758** | 0.1963** | 0.3458*** | 0.4681*** | 0.4350*** |
(3.21) | (2.25) | (2.16) | (2.85) | (4.88) | (5.22) | |
CI | 0.159 | 0.0982** | 0.0954 | 0.1408 | 0.2881** | 0.4066*** |
(1.65) | (2.42) | (1.36) | (1.46) | (2.53) | (3.34) | |
FDI | 5.427** | 8.6024*** | 7.7062*** | 6.3488*** | 4.9094*** | 3.3846*** |
(1.99) | (5.15) | (4.85) | (4.09) | (3.84) | (3.03) | |
T | -0.0221*** | -0.2610*** | -0.2528*** | -0.2087*** | -0.0922 | -0.0182 |
(-4.80) | (-4.48) | (-3.68) | (-2.71) | (-1.12) | (-0.41) | |
UB | 0.0426*** | 0.0347*** | 0.0377*** | 0.0474*** | 0.0672*** | 0.0836*** |
(4.79) | (4.77) | (4.9) | (5.4) | (5.98) | (6.77) | |
ROD | 0.0435*** | 0.0301*** | 0.0248*** | 0.0187*** | 0.0092 | 0.00349 |
(6.04) | (3.17) | (3.06) | (2.64) | (1.42) | (0.65) | |
Cons | -6.114*** | -4.4682*** | -4.5841*** | -4.3932*** | -3.0907** | -1.9161* |
(-4.91) | (-3.14) | (-3.58) | (-3.76) | (-2.54) | (-1.71) | |
N | 6226 | 6226 | 6226 | 6226 | 6226 | 6226 |
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