|
2,500 Monte Carlo runs
2500 is not a good number of runs for a Monte Carlo experiment.
It's interesting as it shows why by the lack of precision.
On other pages, you can see results with
6,250,000 runs, 125,000 runs
and 50 runs.
For further details, e-mail me at
gbel@math.creuset.org.
| Table 1:
yt = θ exp{σ εt },
σ = 1 known. |
| θ0 |
θML |
θAML |
θFS1 |
θFS4 |
θFS5 |
0.5 (0.1) |
0.51223 (0.10112) |
0.50209 (0.09912) |
0.51170 (0.10102) |
0.50204 (0.09912) |
0.50229 (0.10056) |
1.0 (0.2) |
1.01978 (0.20574) |
0.99959 (0.20166) |
1.01873 (0.20553) |
0.99956 (0.20167) |
1.00053 (0.20543) |
1.5 (0.3) |
1.53578 (0.31398) |
1.50537 (0.30776) |
1.53420 (0.31366) |
1.50534 (0.30776) |
1.50463 (0.31506) |
2.0 (0.4) |
2.03347 (0.40345) |
1.99321 (0.39546) |
2.03138 (0.40304) |
1.99321 (0.39550) |
1.99565 (0.40288) |
2.5 (0.5) |
2.54231 (0.51420) |
2.49197 (0.50402) |
2.53970 (0.51368) |
2.49199 (0.50398) |
2.49466 (0.50914) |
| Table 2.1:
yt = θ exp{σ εt },
σ 0 = 0.5 unknown. |
| θ0 |
θML |
θAML |
θFS4 |
θFS5 |
0.5 (0.05) |
0.50276 (0.05129) |
0.49827 (0.04958) |
0.50014 (0.05107) |
0.50022 (0.05123) |
1.0 (0.10) |
1.00535 (0.10089) |
1.00284 (0.09952) |
1.00034 (0.10039) |
1.00060 (0.10059) |
1.5 (0.15) |
1.50963 (0.14955) |
1.49751 (0.15227) |
1.50206 (0.14880) |
1.50237 (0.14968) |
2.0 (0.20) |
2.00606 (0.20355) |
1.99358 (0.20040) |
1.99595 (0.20241) |
1.99603 (0.20238) |
2.5 (0.25) |
2.51146 (0.25647) |
2.50793 (0.24968) |
2.49883 (0.25521) |
2.49896 (0.25580) |
| Table 2.2:
yt = θ exp{σ εt },
σ 0 = 1.0 unknown. |
| θ0 |
θML |
θAML |
θFS4 |
θFS5 |
0.5 (0.10) |
0.50840 (0.10250) |
0.49821 (0.10108) |
0.49822 (0.10057) |
0.49838 (0.10144) |
1.0 (0.20) |
1.02444 (0.20183) |
0.99999 (0.20163) |
1.00425 (0.19776) |
1.00415 (0.20033) |
1.5 (0.30) |
1.53199 (0.31068) |
1.50652 (0.29934) |
1.50211 (0.30519) |
1.50203 (0.30798) |
2.0 (0.40) |
2.03803 (0.40401) |
1.99906 (0.41070) |
1.99749 (0.39614) |
1.99867 (0.40139) |
2.5 (0.50) |
2.54391 (0.52659) |
2.49770 (0.52327) |
2.49338 (0.51614) |
2.49334 (0.52003) |
| Table 2.3:
yt = θ exp{σ εt },
σ 0 = 1.5 unknown. |
| θ0 |
θML |
θAML |
θFS4 |
θFS5 |
0.5 (0.15) |
0.52065 (0.15704) |
0.50009 (0.15542) |
0.49739 (0.15004) |
0.49743 (0.15776) |
1.0 (0.30) |
1.03803 (0.30413) |
0.98368 (0.29753) |
0.99246 (0.29098) |
0.99000 (0.30252) |
1.5 (0.45) |
1.56771 (0.48856) |
1.50034 (0.47046) |
1.49896 (0.46704) |
1.49560 (0.48407) |
2.0 (0.60) |
2.10651 (0.66585) |
1.99064 (0.62739) |
2.01334 (0.63729) |
2.01417 (0.66116) |
2.5 (0.75) |
2.61897 (0.81643) |
2.50838 (0.77502) |
2.50432 (0.78221) |
2.50331 (0.82052) |
| Table 2.4:
yt = θ exp{σ εt },
σ 0 = 2.0 unknown. |
| θ0 |
θML |
θAML |
θFS4 |
θFS5 |
0.5 (0.20) |
0.54464 (0.22501) |
0.49919 (0.20731) |
0.50315 (0.20858) |
0.50459 (0.23298) |
1.0 (0.40) |
1.08059 (0.45786) |
0.99890 (0.43066) |
0.99778 (0.42498) |
0.99809 (0.46686) |
1.5 (0.60) |
1.60321 (0.66159) |
1.48929 (0.62482) |
1.48095 (0.61393) |
1.47558 (0.67438) |
2.0 (0.80) |
2.14718 (0.92240) |
2.01366 (0.87174) |
1.98080 (0.85270) |
1.97896 (0.93936) |
2.5 (1.00) |
2.72250 (1.11931) |
2.50334 (1.02916) |
2.51330 (1.03418) |
2.51107 (1.17331) |
| Table 2.5:
yt = θ exp{σ εt },
σ 0 = 2.5 unknown. |
| θ0 |
θML |
θAML |
θFS4 |
θFS5 |
0.5 (0.25) |
0.56794 (0.30818) |
0.49902 (0.26829) |
0.50159 (0.27315) |
0.49787 (0.38587) |
1.0 (0.50) |
1.11136 (0.57032) |
1.00467 (0.55106) |
0.98117 (0.50560) |
0.98139 (0.68912) |
1.5 (0.75) |
1.69056 (0.91670) |
1.50245 (0.80672) |
1.49076 (0.81242) |
1.46686 (1.07566) |
2.0 (1.00) |
2.27930 (1.24934) |
1.98035 (1.07199) |
2.01314 (1.11184) |
2.01675 (1.45688) |
2.5 (1.25) |
2.78886 (1.47016) |
2.52604 (1.38458) |
2.46253 (1.29890) |
2.49240 (1.78469) |
| Table 2.6:
yt = θ exp{σ εt },
θ0 = 0.5 unknown. |
| σ0 |
σML |
σAML |
σFS4 |
σFS5 |
0.5 (0.07071) |
0.48335 (0.06930) |
0.50532 (0.07245) |
0.49847 (0.07148) |
0.49860 (0.07368) |
1.0 (0.14142) |
0.97113 (0.13903) |
1.01180 (0.15099) |
1.00155 (0.14338) |
1.00175 (0.14723) |
1.5 (0.21213) |
1.46455 (0.21401) |
1.52110 (0.22503) |
1.51041 (0.22072) |
1.50986 (0.22626) |
2.0 (0.28284) |
1.93671 (0.27623) |
2.02728 (0.29317) |
1.99735 (0.28486) |
1.99673 (0.29230) |
2.5 (0.35355) |
2.41842 (0.34756) |
2.51949 (0.35470) |
2.49405 (0.35836) |
2.49631 (0.36957) |
| Table 2.7:
yt = θ exp{σ εt },
θ0 = 1.0 unknown. |
| σ0 |
σML |
σAML |
σFS4 |
σFS5 |
0.5 (0.07071) |
0.48451 (0.07032) |
0.50124 (0.07374) |
0.49966 (0.07251) |
0.49938 (0.07401) |
1.0 (0.14142) |
0.96835 (0.14419) |
1.01577 (0.14177) |
0.99864 (0.14870) |
0.99832 (0.15302) |
1.5 (0.21213) |
1.45397 (0.21041) |
1.50981 (0.22335) |
1.49944 (0.21696) |
1.50142 (0.22389) |
2.0 (0.28284) |
1.93898 (0.27880) |
2.01702 (0.29545) |
1.99955 (0.28747) |
2.00223 (0.29672) |
2.5 (0.35355) |
2.41844 (0.35049) |
2.53427 (0.38289) |
2.49402 (0.36149) |
2.49637 (0.37300) |
| Table 2.8:
yt = θ exp{σ εt },
θ0 = 1.5 unknown. |
| σ0 |
σML |
σAML |
σFS4 |
σFS5 |
0.5 (0.07071) |
0.48254 (0.06861) |
0.50381 (0.07320) |
0.49763 (0.07075) |
0.49762 (0.07292) |
1.0 (0.14142) |
0.96510 (0.13979) |
1.01012 (0.14608) |
0.99531 (0.14418) |
0.99570 (0.14655) |
1.5 (0.21213) |
1.44954 (0.21023) |
1.51340 (0.22600) |
1.49492 (0.21678) |
1.49689 (0.22312) |
2.0 (0.28284) |
1.92994 (0.28759) |
2.01791 (0.28875) |
1.99026 (0.29656) |
1.99154 (0.30386) |
2.5 (0.35355) |
2.43020 (0.34709) |
2.52702 (0.35964) |
2.50623 (0.35806) |
2.50681 (0.36701) |
| Table 2.9:
yt = θ exp{σ εt },
θ0 = 2.0 unknown. |
| σ0 |
σML |
σAML |
σFS4 |
σFS5 |
0.5 (0.07071) |
0.48415 (0.07037) |
0.50395 (0.07219) |
0.49928 (0.07257) |
0.49944 (0.07449) |
1.0 (0.14142) |
0.97146 (0.14227) |
1.00896 (0.14395) |
1.00190 (0.14675) |
1.00155 (0.15117) |
1.5 (0.21213) |
1.45833 (0.20851) |
1.51507 (0.22738) |
1.50399 (0.21501) |
1.50296 (0.22197) |
2.0 (0.28284) |
1.94861 (0.28514) |
2.01463 (0.29041) |
2.00963 (0.29403) |
2.00908 (0.30248) |
2.5 (0.35355) |
2.42512 (0.36102) |
2.52457 (0.37163) |
2.50087 (0.37234) |
2.50085 (0.38166) |
| Table 2.10:
yt = θ exp{σ εt },
θ0 = 2.5 unknown. |
| σ0 |
σML |
σAML |
σFS4 |
σFS5 |
0.5 (0.07071) |
0.48448 (0.07073) |
0.50656 (0.07334) |
0.49962 (0.07295) |
0.49959 (0.07505) |
1.0 (0.14142) |
0.97055 (0.13983) |
1.01135 (0.14838) |
1.00096 (0.14421) |
1.00026 (0.14712) |
1.5 (0.21213) |
1.45362 (0.20808) |
1.50972 (0.22176) |
1.49902 (0.21452) |
1.49997 (0.22037) |
2.0 (0.28284) |
1.94169 (0.28657) |
2.01326 (0.30084) |
2.00253 (0.29559) |
2.00463 (0.30191) |
2.5 (0.35355) |
2.41770 (0.36625) |
2.51833 (0.37409) |
2.49333 (0.37834) |
2.49182 (0.38075) |
| Table 3:
zt = 1[yt > 0],
yt = α + xt β + &epsilont |
| β0 |
βOLS / σOLS |
&betaFS4 |
-1.0 (0.46906) |
-0.94988 (0.27061) |
-1.00669 (0.34704) |
-0.5 (0.42959) |
-0.56031 (0.33883) |
-0.49936 (0.31079) |
0.0 (0.41713) |
-0.01472 (0.37046) |
-0.00942 (0.29448) |
0.5 (0.42959) |
0.56639 (0.33136) |
0.51314 (0.30572) |
1.0 (0.46906) |
0.94951 (0.26512) |
0.99237 (0.27362) |
|