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Table 8 NARDL long run and short run estimates (daily number of new reported COVID-19 cases worldwide included)

From: Exploring the asymmetric effect of COVID-19 pandemic news on the cryptocurrency market: evidence from nonlinear autoregressive distributed lag approach and frequency domain causality

Model 1

Model 2

Model 3

Model 4

Model 5

Model 6

\(\mathrm{ECT}\)

−1.090046*** (0.042107)

\(\mathrm{ECT}\)

−1.095174*** (0.042679)

\(\mathrm{ECT}\)

−1.132591*** (0.042498)

\(\mathrm{ECT}\)

−1.11978*** (0.042515)

\(\mathrm{ECT}\)

−1.094086*** (0.042804)

\(\mathrm{ECT}\)

−1.096896*** (0.042919)

Long-run and short-run coefficients

Const

0.011766 (0.02905)

Const

0.003942 (0.031316)

Const

−0.00041 (0.027761)

Const

0.01041 (0.022178)

Const

0.016295 (0.0315)

Const

−0.014911 (0.027113)

\({\mathrm{BTC}}_{\mathrm{t}-1}\)

−1.090046*** (0.046904)

\({\mathrm{BTC}}_{\mathrm{t}-1}\)

−1.095174*** (0.047337)

\({\mathrm{BTC}}_{\mathrm{t}-1}\)

−1.132591*** (0.047067)

\({\mathrm{BTC}}_{\mathrm{t}-1}\)

−1.11978*** (0.046833)

\({\mathrm{BTC}}_{\mathrm{t}-1}\)

−1.094086*** (0.047676)

\({\mathrm{BTC}}_{\mathrm{t}-1}\)

−1.096896*** (0.047675)

\({\mathrm{PI}}^{+}\)

0.008929*** (0.002856)

\({\mathrm{HI}}^{+}\)

0.000896* (0.000499)

\({\mathrm{FNI}}^{+}\)

0.039701*** (0.010661)

\({\mathrm{SI}}_{\mathrm{t}-1}^{+}\)

−0.000149 (0.00018)

\({\mathrm{II}}^{+}\)

0.001655* (0.000848)

\({\mathrm{MCI}}^{+}\)

0.001342* (0.000722)

\({\mathrm{PI}}^{-}\)

0.00764*** (0.002485)

\({\mathrm{HI}}^{-}\)

0.000766** (0.000329)

\({\mathrm{FNI}}_{\mathrm{t}-1}^{-}\)

0.03784*** (0.010433)

\({\mathrm{SI}}^{-}\)

−0.00022* (0.00013)

\({\mathrm{II}}_{\mathrm{t}-1}^{-}\)

0.001329* (0.000688)

\({\mathrm{MCI}}^{-}\)

0.000859 (0.00057)

\({\mathrm{CNC}}_{\mathrm{t}-1}^{+}\)

−0.004168 (0.004575)

\({\mathrm{CNC}}_{\mathrm{t}-1}^{+}\)

−0.005491 (0.007048)

\({\mathrm{CNC}}_{\mathrm{t}-1}^{+}\)

−0.000792 (0.003991)

\({\mathrm{CNC}}^{+}\)

0.003035 (0.004543)

\({\mathrm{CNC}}_{\mathrm{t}-1}^{+}\)

−0.010901 (0.008179)

\({\mathrm{CNC}}_{\mathrm{t}-1}^{+}\)

−0.006703 (0.006833)

\({\mathrm{CNC}}_{\mathrm{t}-1}^{-}\)

−0.000471 (0.003542)

\({\mathrm{CNC}}_{\mathrm{t}-1}^{-}\)

−0.001544 (0.006103)

\({\mathrm{CNC}}_{\mathrm{t}-1}^{-}\)

0.004079 (0.00284)

\({\mathrm{CNC}}^{-}\)

0.007222* (0.004311)

\({\mathrm{CNC}}_{\mathrm{t}-1}^{-}\)

−0.007015 (0.006038)

\({\mathrm{CNC}}_{\mathrm{t}-1}^{-}\)

−0.003014 (0.004615)

\({\mathrm{VIX}}^{+}\)

−0.164421*** (0.02411)

\({\mathrm{VIX}}^{+}\)

−0.157511*** (0.024488)

\({\mathrm{VIX}}^{+}\)

−0.161608*** (0.023664)

\({\mathrm{VIX}}^{+}\)

−0.1567*** (0.023642)

\({\mathrm{VIX}}^{+}\)

−0.164333*** (0.024033)

\({\mathrm{VIX}}^{+}\)

−0.16386*** (0.024246)

\({\mathrm{VIX}}^{-}\)

−0.163397*** (0.022702)

\({\mathrm{VIX}}^{-}\)

−0.162211*** (0.022835)

\({\mathrm{VIX}}^{-}\)

−0.163935*** (0.022708)

\({\mathrm{VIX}}^{-}\)

−0.158306*** (0.022925)

\({\mathrm{VIX}}^{-}\)

−0.164061*** (0.022973)

\({\mathrm{VIX}}^{-}\)

−0.163882*** (0.022868)

\(\Delta {\mathrm{CNC}}^{+}\)

0.028717** (0.014535)

\(\Delta {\mathrm{CNC}}^{+}\)

0.032861** (0.014497)

\(\Delta {\mathrm{FNI}}^{+}\)

0.025312** (0.012096)

\(\Delta {\mathrm{SI}}^{+}\)

0.000807* (0.000483)

\(\Delta {\mathrm{II}}^{-}\)

−0.00105 (0.00129)

\(\Delta {\mathrm{CNC}}^{+}\)

0.031113** (0.014683)

\(\Delta {\mathrm{CNC}}_{\mathrm{t}-1}^{+}\)

−0.023874* (0.013517)

\(\Delta {\mathrm{CNC}}_{\mathrm{t}-1}^{+}\)

−0.021712 (0.014058)

\(\Delta {\mathrm{FNI}}_{\mathrm{t}-1}^{+}\)

−0.037215** (0.016586)

  

\(\Delta {\mathrm{CNC}}^{+}\)

0.029177** (0.014815)

\(\Delta {\mathrm{CNC}}_{\mathrm{t}-1}^{+}\)

−0.021358 (0.013731)

\(\Delta {\mathrm{CNC}}_{\mathrm{t}-2}^{+}\)

0.025533** (0.011109)

\(\Delta {\mathrm{CNC}}_{\mathrm{t}-2}^{+}\)

0.028266** (0.011359)

\(\Delta {\mathrm{FNI}}^{-}\)

−0.016338 (0.016756)

  

\(\Delta {\mathrm{CNC}}_{\mathrm{t}-1}^{+}\)

−0.016774 (0.014142)

\(\Delta {\mathrm{CNC}}_{\mathrm{t}-2}^{+}\)

0.027311** (0.011297)

\(\Delta {\mathrm{CNC}}^{-}\)

−0.001122 (0.014702)

\(\Delta {\mathrm{CNC}}^{-}\)

−0.008519 (0.014833)

\(\Delta {\mathrm{CNC}}^{+}\)

0.028241** (0.014226)

  

\(\Delta {\mathrm{CNC}}_{\mathrm{t}-2}^{+}\)

0.028706** (0.011464)

\(\Delta {\mathrm{CNC}}^{-}\)

−0.012482 (0.015553)

\(\Delta {\mathrm{CNC}}_{\mathrm{t}-1}^{-}\)

0.039652** (0.018272)

\(\Delta {\mathrm{CNC}}_{\mathrm{t}-1}^{-}\)

0.043047** (0.018396)

\(\Delta {\mathrm{CNC}}_{\mathrm{t}-1}^{+}\)

−0.019469 (0.013647)

  

\(\Delta {\mathrm{CNC}}^{-}\)

−0.002625 (0.016823)

\(\Delta {\mathrm{CNC}}_{\mathrm{t}-1}^{-}\)

0.040951** (0.018305)

\(\Delta {\mathrm{CNC}}_{\mathrm{t}-2}^{-}\)

−0.040723** (0.017395)

\(\Delta {\mathrm{CNC}}_{\mathrm{t}-2}^{-}\)

−0.041628** (0.017463)

\(\Delta {\mathrm{CNC}}^{-}\)

−0.011874 (0.015298)

  

\(\Delta {\mathrm{CNC}}_{\mathrm{t}-1}^{-}\)

0.041516** (0.018362)

\(\Delta {\mathrm{CNC}}_{\mathrm{t}-2}^{-}\)

−0.040451** (0.017309)

    

\(\Delta {\mathrm{CNC}}_{\mathrm{t}-1}^{-}\)

0.03323* (0.017541)

  

\(\Delta {\mathrm{CNC}}_{\mathrm{t}-2}^{-}\)

−0.036842** (0.017236)

  
    

\(\Delta {\mathrm{CNC}}_{\mathrm{t}-2}^{-}\)

−0.026595 (0.016372)

      
    

\(\Delta {\mathrm{CNC}}_{\mathrm{t}-3}^{-}\)

−0.032454** (0.013145)

      

Long-run asymmetric effects

\({\mathrm{L}}_{\mathrm{PI}}^{+}\)

0.008191*** (0.002634)

\({\mathrm{L}}_{\mathrm{HI}}^{+}\)

0.000818* (0.000455)

\({\mathrm{L}}_{\mathrm{FNI}}^{+}\)

0.035054*** (0.00931)

\({\mathrm{L}}_{\mathrm{SI}}^{+}\)

−0.000133 (0.00016)

\({\mathrm{L}}_{\mathrm{II}}^{+}\)

0.001512* (0.00077)

\({\mathrm{L}}_{\mathrm{MCI}}^{+}\)

0.001223* (0.000654)

\({\mathrm{L}}_{\mathrm{PI}}^{-}\)

0.007009*** (0.00229)

\({\mathrm{L}}_{\mathrm{HI}}^{-}\)

0.0007** (0.000299)

\({\mathrm{L}}_{\mathrm{FNI}}^{-}\)

0.03341*** (0.009118)

\({\mathrm{L}}_{\mathrm{SI}}^{-}\)

−0.000196* (0.000116)

\({\mathrm{L}}_{\mathrm{II}}^{-}\)

0.001215* (0.000625)

\({\mathrm{L}}_{\mathrm{MCI}}^{-}\)

0.000783 (0.000516)

\({\mathrm{L}}_{\mathrm{CNC}}^{+}\)

−0.003823 (0.004201)

\({\mathrm{L}}_{\mathrm{CNC}}^{+}\)

−0.005014 (0.006435)

\({\mathrm{L}}_{\mathrm{CNC}}^{+}\)

−0.0007 (0.003524)

\({\mathrm{L}}_{\mathrm{CNC}}^{+}\)

0.002711 (0.004055)

\({\mathrm{L}}_{\mathrm{CNC}}^{+}\)

−0.009964 (0.007447)

\({\mathrm{L}}_{\mathrm{CNC}}^{+}\)

−0.006111 (0.006208)

\({\mathrm{L}}_{\mathrm{CNC}}^{-}\)

−0.000432 (0.00325)

\({\mathrm{L}}_{\mathrm{CNC}}^{-}\)

−0.00141 (0.005575)

\({\mathrm{L}}_{\mathrm{CNC}}^{-}\)

0.003602 (0.002496)

\({\mathrm{L}}_{\mathrm{CNC}}^{-}\)

0.006449* (0.00383)

\({\mathrm{L}}_{\mathrm{CNC}}^{-}\)

−0.006411 (0.00551)

\({\mathrm{L}}_{\mathrm{CNC}}^{-}\)

−0.002748 (0.004203)

\({\mathrm{L}}_{\mathrm{VIX}}^{+}\)

−0.150839*** (0.023894)

\({\mathrm{L}}_{\mathrm{VIX}}^{+}\)

−0.143823*** (0.024099)

\({\mathrm{L}}_{\mathrm{VIX}}^{+}\)

−0.142689*** (0.022549)

\({\mathrm{L}}_{\mathrm{VIX}}^{+}\)

−0.139938*** (0.022723)

\({\mathrm{L}}_{\mathrm{VIX}}^{+}\)

−0.150201*** (0.023827)

\({\mathrm{L}}_{\mathrm{VIX}}^{+}\)

−0.149385*** (0.023932)

\({\mathrm{L}}_{\mathrm{VIX}}^{-}\)

−0.1499*** (0.022607)

\({\mathrm{L}}_{\mathrm{VIX}}^{-}\)

−0.148114*** (0.022629)

\({\mathrm{L}}_{\mathrm{VIX}}^{-}\)

−0.144743*** (0.02174)

\({\mathrm{L}}_{\mathrm{VIX}}^{-}\)

−0.141372*** (0.022083)

\({\mathrm{L}}_{\mathrm{VIX}}^{-}\)

−0.149953*** (0.022858)

\({\mathrm{L}}_{\mathrm{VIX}}^{-}\)

−0.149405*** (0.022651)

Const

0.010794 (0.026645)

Const

0.003599 (0.028592)

Const

−0.000362 (0.024511)

Const

0.009296 (0.019797)

Const

0.014894 (0.028755)

Const

−0.013594 (0.024736)

Long run asymmetry tests – Wald statistics

\({\mathrm{W}}_{\mathrm{LR}}(\mathrm{PI})\)

4.487301**

\({\mathrm{W}}_{\mathrm{LR}}(\mathrm{HI})\)

0.3338

\({\mathrm{W}}_{\mathrm{LR}}(\mathrm{FNI})\)

2.139061

\({\mathrm{W}}_{\mathrm{LR}}(\mathrm{SI})\)

0.148092

\({\mathrm{W}}_{\mathrm{LR}}(\mathrm{II})\)

4.581732**

\({\mathrm{W}}_{\mathrm{LR}}(\mathrm{MCI})\)

1.265293

\({\mathrm{W}}_{\mathrm{LR}}(\mathrm{CNC})\)

2.739795*

\({\mathrm{W}}_{\mathrm{LR}}(\mathrm{CNC})\)

3.337275*

\({\mathrm{W}}_{\mathrm{LR}}(\mathrm{CNC})\)

2.451346

\({\mathrm{W}}_{\mathrm{LR}}(\mathrm{CNC})\)

1.772852

\({\mathrm{W}}_{\mathrm{LR}}(\mathrm{CNC})\)

3.37373*

\({\mathrm{W}}_{\mathrm{LR}}(\mathrm{CNC})\)

3.355494*

\({\mathrm{W}}_{\mathrm{LR}}(\mathrm{VIX})\)

0.001809

\({\mathrm{W}}_{\mathrm{LR}}(\mathrm{VIX})\)

1.109015

\({\mathrm{W}}_{\mathrm{LR}}(\mathrm{VIX})\)

0.316811

\({\mathrm{W}}_{\mathrm{LR}}(\mathrm{VIX})\)

0.188459

\({\mathrm{W}}_{\mathrm{LR}}(\mathrm{VIX})\)

0.113445

\({\mathrm{W}}_{\mathrm{LR}}(\mathrm{VIX})\)

0.4769

Statistics and diagnostics

R-sq

0.190674

R−sq

0.18174

R−sq

0.215594

R−sq

0.158729

R−sq

0.179996

R−sq

0.177612

Adj R-sq

0.163765

Adj R−sq

0.154534

Adj R−sq

0.183163

Adj R−sq

0.14182

Adj R−sq

0.15056

Adj R−sq

0.150269

F-stat

7.085999***

F−stat

6.680244***

F−stat

6.647919***

F−stat

9.386746***

F−stat

6.114826***

F−stat

6.495744***

D-W stat

2.060461

D−W stat

2.058759

D−W stat

2.044533

D−W stat

2.03404

D−W stat

2.063541

D−W stat

2.070825

\({\upchi }_{\mathrm{SC}}^{2} (1)\)

2.366963 [0.1247]

\({\upchi }_{\mathrm{SC}}^{2} (1)\)

2.467295 [0.117]

\({\upchi }_{\mathrm{SC}}^{2} (1)\)

1.263353 [0.2617]

\({\upchi }_{\mathrm{SC}}^{2} (1)\)

1.098021 [0.2953]

\({\upchi }_{\mathrm{SC}}^{2} (1)\)

2.856843 [0.0918]

\({\upchi }_{\mathrm{SC}}^{2} (1)\)

3.44255 [0.0643]

\({\upchi }_{\mathrm{SC}}^{2} (2)\)

1.217663 [0.297]

\({\upchi }_{\mathrm{SC}}^{2} (2)\)

1.238976 [0.2908]

\({\upchi }_{\mathrm{SC}}^{2} (2)\)

0.816957 [0.4425]

\({\upchi }_{\mathrm{SC}}^{2} (2)\)

0.552424 [0.576]

\({\upchi }_{\mathrm{SC}}^{2} (2)\)

1.441961 [0.2377]

\({\upchi }_{\mathrm{SC}}^{2} (2)\)

1.756983 [0.1739]

\({\upchi }_{\mathrm{HET}}^{2} (1)\)

0.118551 [0.7308]

\({\upchi }_{\mathrm{HET}}^{2} (1)\)

0.050962 [0.8215]

\({\upchi }_{\mathrm{HET}}^{2} (1)\)

0.090182 [0.7641]

\({\upchi }_{\mathrm{HET}}^{2} (1)\)

0.003739 [0.9513]

\({\upchi }_{\mathrm{HET}}^{2} (1)\)

0.016026 [0.8993]

\({\upchi }_{\mathrm{HET}}^{2} (1)\)

0.047376 [0.8278]

\({\upchi }_{\mathrm{HET}}^{2} (2)\)

0.062791 [0.9391]

\({\upchi }_{\mathrm{HET}}^{2} (2)\)

0.031419 [0.9691]

\({\upchi }_{\mathrm{HET}}^{2} (2)\)

0.045698 [0.9553]

\({\upchi }_{\mathrm{HET}}^{2} (2)\)

0.004194 [0.9958]

\({\upchi }_{\mathrm{HET}}^{2} (2)\)

0.008891 [0.9911]

\({\upchi }_{\mathrm{HET}}^{2} (2)\)

0.02622 [0.9741]

\({\upchi }_{\mathrm{NORM}}^{2}\)

1196.586 [0.0000]

\({\upchi }_{\mathrm{NORM}}^{2}\)

1146.037 [0.0000]

\({\upchi }_{\mathrm{NORM}}^{2}\)

1337.827 [0.0000]

\({\upchi }_{\mathrm{NORM}}^{2}\)

1381.666 [0.0000]

\({\upchi }_{\mathrm{NORM}}^{2}\)

1056.104 [0.0000]

\({\upchi }_{\mathrm{NORM}}^{2}\)

1240.097 [0.0000]

\({\upchi }_{\mathrm{RESET}}^{2}\)

0.364455 [0.5464]

\({\upchi }_{\mathrm{RESET}}^{2}\)

0.007184 [0.9325]

\({\upchi }_{\mathrm{RESET}}^{2}\)

0.174737 [0.6762]

\({\upchi }_{\mathrm{RESET}}^{2}\)

0.075537 [0.7836]

\({\upchi }_{\mathrm{RESET}}^{2}\)

0.754172 [0.4512]

\({\upchi }_{\mathrm{RESET}}^{2}\)

0.106922 [0.9149]

  1. Source Authors’ own computations. Notes: Superscripts *, **, *** represent the significance at 10%, 5%, and 1% levels, respectively. The superscript + and – defines positive and negative partial sum. \({\mathrm{L}}^{+}\) and \({\mathrm{L}}^{-}\) are the computed long-run coefficients associated with positive and negative shocks, respectively. \({\mathrm{W}}_{\mathrm{LR}}\) denotes the Wald statistic for the long-run symmetry. \({\mathrm{W}}_{\mathrm{LR}}\) denotes the Wald statistic for the long-run symmetry, which tests the null hypothesis of \({\theta }^{+}\) =\({\theta }^{-}\). \({\mathrm{\rm X}}_{\mathrm{SC}}^{2}\) denotes the Breusch-Godfrey Serial Correlation LM Test (first and second lag). \({\mathrm{\rm X}}_{\mathrm{HET}}^{2}\) denotes the Heteroskedasticity Test: ARCH (first and second lag). \({\mathrm{\rm X}}_{\mathrm{RESET}}^{2}\) denotes the Ramsey RESET Test of Misspecification. \({\mathrm{\rm X}}_{\mathrm{NORM}}^{2}\) denotes the Jarque–Bera test. The p-values of diagnostic tests are in []. Variables’ description is provided in Table 4