| Literature DB >> 35975113 |
Zeyi Fu1, Hongli Niu1, Weiqing Wang1.
Abstract
Despite the upgrading of the attention and investment of new energy in Chinese public, its market efficiency and associations with other assets are relatively rarely explored. This paper, firstly, explores the multifractal feature and market efficiency of Chinese new energy market (NEI) by the multifractal detrended fluctuation analysis. Secondly, the multifractal cross-correlation analysis is performed to discuss the multifractality of cross-correlations between NEI and crude oil, external new energy indices (Global (SPGCE), United States (ECO) and Europe (ERIX)) and safe-haven asset (GOLD) respectively. The results show that Chinese new energy market has obvious multifractality with low market efficiency, which is mainly sourced from long-range correlation. It has the strongest linkages with external new energy markets and most insignificant association with gold. The heterogeneous sources contribute to their multifractal cross-correlations. It provides useful enlightenment for decision-makers to implement energy policy and reform, and for investors to make investment decisions.Entities:
Keywords: Cross-correlation; Market efficiency; Multifractal sources; Multifractality; New energy market
Year: 2022 PMID: 35975113 PMCID: PMC9371636 DOI: 10.1007/s10614-022-10301-2
Source DB: PubMed Journal: Comput Econ ISSN: 0927-7099 Impact factor: 1.741
Fig. 1Daily prices of NEI (including log return) and other six indicators from 2009.10.28 to 2021.03.31
Descriptive statistics of indicators
| NEI | DAQ | GOLD | WTI | SPGCE | ECO | ERIX | |
|---|---|---|---|---|---|---|---|
| Mean | 0.0002 | − 0.0001 | 0.0002 | 0.0001 | 0.0000 | 0.0003 | 0.0004 |
| Maximum | 0.0803 | 0.2955 | 0.0519 | 0.3196 | 0.1463 | 0.1501 | 0.1036 |
| Minimum | − 0.0983 | − 0.3617 | − 0.0947 | − 0.2822 | − 0.1250 | − 0.1594 | − 0.1297 |
| Std.Dev | 0.0199 | 0.0272 | 0.0099 | 0.0277 | 0.0161 | 0.0207 | 0.0168 |
| Skewness | − 0.6371 | − 0.7162 | − 0.5814 | 0.2373 | − 0.2349 | − 0.2950 | − 0.3165 |
| Kurtosis | 5.9893 | 34.3670 | 10.6978 | 31.1815 | 12.6753 | 10.6165 | 7.6979 |
| J-B Stat | 1152.3a | 107,590.8a | 6613.9a | 86,625.0a | 10,239.4a | 6368.4a | 2452.2a |
| Obs | 2619 | 2619 | 2619 | 2619 | 2619 | 2619 | 2619 |
aDenotes the test is statistically significant at the 99% level of confidence
Fig. 2Multifractal characteristic of NEI
Fig. 3The generalized Hurst exponents and multifractal spectra of the original, shuffled, staggered and Evremoved series
The multifractal features of the original, shuffled, staggered and Evremoved series
| Original series | Shuffled series | Staggered series | EVremoved series | |
|---|---|---|---|---|
| 0.5338 | 0.5182 | 0.4999 | 0.4620 | |
| 0.4471 | 0.1411 | 0.3856 | 0.4100 | |
| 0.6014 | 0.2420 | 0.5169 | 0.4832 |
Fig. 4The cross-correlation statistics for the six pairs of variables
Fig. 5DCCA coefficients of six pairs of assets for different scale s
Fig. 6The log–log plots of versus s for NEI and other six assets
Fig. 7Multifractal characteristic of cross-correlation for NEI and other six assets
The multifractal degree of cross-correlation for NEI and other six assets
| NEI-DAQ | NEI-GOLD | NEI-WTI | NEI-SPGCE | NEI-ECO | NEI-ERIX | |
|---|---|---|---|---|---|---|
| 0.1813 | 0.1639 | 0.2737 | 0.1760 | 0.0396 | 0.2755 | |
| 0.3104 | 0.2579 | 0.4516 | 0.2785 | 0.0743 | 0.4188 |
The source analysis of multifractality of six pairs of cross-correlation
| Original | Shuffled | Staggered | EVremoved | Original | Shuffled | Staggered | EVremoved | ||
|---|---|---|---|---|---|---|---|---|---|
| NEI-DAQ | NEI-GOLD | ||||||||
| | 0.1813 | 0.0800 | 0.0477 | 0.0462 | 0.1638 | 0.1471 | 0.1037 | 0.0940 | |
| | 0.3104 | 0.1747 | 0.1400 | 0.1168 | 0.2579 | 0.2473 | 0.1790 | 0.1608 | |
| NEI-WTI | NEI-SPGCE | ||||||||
| | 0.2737 | 0.2002 | 0.0425 | 0.1163 | 0.1761 | 0.1163 | 0.1219 | 0.1665 | |
| | 0.4516 | 0.3394 | 0.1152 | 0.1915 | 0.2786 | 0.2042 | 0.2239 | 0.2764 | |
| NEI-ECO | NEI-ERIX | ||||||||
| | 0.0396 | 0.1456 | 0.0264 | 0.0549 | 0.2756 | 0.0489 | 0.2034 | 0.2318 | |
| | 0.0743 | 0.2365 | 0.0443 | 0.1084 | 0.4189 | 0.1010 | 0.3462 | 0.4199 | |