Hi Nils,
Please find attached data for U=15 and higher T. The only problem is
that as T is increased there are less available common temperatures for
the different dtau.
I have just returned form vacations, so I will be able to reply faster
from now on.
Happy New Year!
Thereza
On Wed, 15 Dec 2010, Nils Bluemer wrote:
Hi Thereza,
> thank you very much, this is looking great! Attached is a comparison
which shows perfect agreement for the extrapolated data at low T.
> It would be nice to demonstrate agreement also at higher temperatures.
Could you maybe add a few runs (up to T=1 or T=1.25)? We have just
finished our proposal and are now back working on the draft. More soon.
Bests, Nils
On 11.12.2010, at 04:13, Thereza Cristina de Lacerda Paiva wrote:
Hi Nils,
I am sending data for U=15 and four dtau values attached. For
dt=0.05 there are more runs to get a better statistic.
Sorry for the delay!
Thereza
<doccu15l6dt008333.dat><doccu15l6dt005.dat><doccu15l6dt01.dat><doccu15l6dt00625.dat>
Nils Blümer
Institut für Physik, KOMET 337 Room: 03 134, Staudingerweg 7
Johannes Gutenberg-Universität Phone: (+49) 6131 / 392 22 77
55099 Mainz, Germany FAX: (+49) 6131 / 392 09 54
http://komet337.physik.uni-mainz.de/Bluemer/
---------------------------------------------
Thereza Cristina de Lacerda Paiva
Departamento de Fisica dos Solidos
Instituto de Fisica
Universidade Federal do Rio de Janeiro
tclp@if.ufrj.br
www.if.ufrj.br/~tclp/tclp.html
tel: 55 21 2562-7316
fax: 55 21 2562-7368
8 0.100000 0.016417 0.000027
10 0.100000 0.014668 0.000029
12 0.100000 0.014233 0.000038
16 0.100000 0.014545 0.000034
20 0.100000 0.015162 0.000053
30 0.100000 0.016806 0.000091
40 0.100000 0.019083 0.000092
50 0.100000 0.020158 0.000029
60 0.100000 0.020492 0.000044
10 0.083333 0.016707 0.000025
12 0.083333 0.015350 0.000026
16 0.083333 0.014971 0.000024
18 0.083333 0.015036 0.000030
20 0.083333 0.015301 0.000041
24 0.083330 0.015977 0.000054
30 0.083330 0.016820 0.000079
36 0.083330 0.017813 0.000106
42 0.083330 0.018948 0.000073
48 0.083330 0.019973 0.000073
54 0.083330 0.020685 0.000066
60 0.083330 0.021341 0.000039
66 0.083330 0.021643 0.000051
72 0.083330 0.021819 0.000044
12 0.062500 0.018795 0.000027
16 0.062500 0.016292 0.000026
20 0.062500 0.015822 0.000038
24 0.062500 0.015993 0.000057
28 0.062500 0.016290 0.000055
32 0.062500 0.016782 0.000047
40 0.062500 0.017724 0.000069
48 0.062500 0.018612 0.000088
56 0.062500 0.019566 0.000078
64 0.062500 0.020928 0.000121
72 0.062500 0.022013 0.000115
80 0.062500 0.022508 0.000171
88 0.062500 0.023010 0.000055
96 0.062500 0.023284 0.000044
16 0.050000 0.018369 0.000024
20 0.050000 0.016569 0.000029
24 0.050000 0.016145 0.000045
28 0.050000 0.016292 0.000039
30 0.050000 0.016399 0.000063
32 0.050000 0.016530 0.000025
36 0.050000 0.016949 0.000042
40 0.050000 0.017262 0.000069
40 0.050000 0.017295 0.000063
40 0.050000 0.017314 0.000063
40 0.050000 0.017201 0.000074
50 0.050000 0.018361 0.000040
50 0.050000 0.018272 0.000065
50 0.050000 0.018139 0.000061
50 0.050000 0.018329 0.000064
60 0.050000 0.019073 0.000061
60 0.050000 0.018988 0.000080
60 0.050000 0.019222 0.000063
60 0.050000 0.019273 0.000089
70 0.050000 0.020157 0.000120
70 0.050000 0.020205 0.000118
70 0.050000 0.020135 0.000072
70 0.050000 0.020205 0.000096
80 0.050000 0.021706 0.000164
80 0.050000 0.021595 0.000103
80 0.050000 0.021317 0.000067
80 0.050000 0.021535 0.000103
90 0.050000 0.022567 0.000093
90 0.050000 0.022433 0.000082
90 0.050000 0.022518 0.000124
90 0.050000 0.022249 0.000061
100 0.050000 0.023213 0.000076
100 0.050000 0.023313 0.000080
100 0.050000 0.023227 0.000080
100 0.050000 0.023287 0.000043
110 0.050000 0.023686 0.000067
110 0.050000 0.023726 0.000044
110 0.050000 0.023800 0.000059
110 0.050000 0.023686 0.000085
120 0.050000 0.023948 0.000070
120 0.050000 0.023923 0.000043
120 0.050000 0.024004 0.000049
120 0.050000 0.024024 0.000066