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The
Observed Properties of Liquid Helium
at the Saturated Vapor
Pressure
Chapter
13. Dispersion Curve
Adopted Database
Author(s) |
Key # |
Method |
Range(Å-1) |
Svensson et al. |
1 |
Neutron scattering |
0.3
Q
1.13 |
Cowley & Woods |
2 |
" |
0.2
Q
3.6 |
Woods et al. |
3 |
" |
1.9
Q
1.96 |
Stirling et al. |
4 |
" |
0.089
Q
0.8925 |
Stirling |
5 |
" |
1.88
Q
1.97 |
Comments and Key to Authors
1) Ref. 10.
2) Ref. 3.
3) Ref. 7.
4) Ref. 9.
5) Ref. 13.
6) The accuracy of neutron scattering measurements depends very much on
the wavenumber range. It is probably best appreciated by inspecting the
deviation plot in Fig. 13.3. The quantity E is a measure of the energy
of an elementary excitation at a wave number Q. The wave number Q used
here is expressed in reciprocal Ongstroms (=108).
Table
13.1. The adopted database used for the dispersion curve for liquid 4He.
Q(Å-1) |
E/k (K) |
Key |
Q(Å-1) |
E/k (K) |
Key |
0.08940
|
1.61309 |
4 |
1.100 |
13.8000 |
2 |
0.09460 |
1.71754
|
4
|
1.130 |
13.8200 |
1 |
0.1150 |
2.10050 |
4 |
1.200
|
13.7500 |
2 |
0.1210
|
2.25137 |
4
|
1.300
|
13.5000 |
2 |
0.1390 |
2.61112 |
4 |
1.400 |
12.9500
|
2 |
0.1430
|
2.63433 |
4 |
1.500
|
12.2000 |
2 |
0.1594 |
2.97088 |
4 |
1.600 |
11.2000 |
2 |
0.1767 |
3.29582
|
4
|
1.700 |
10.2500 |
2 |
0.1818 |
3.38866 |
4
|
1.800 |
9.25000 |
2 |
0.1938 |
3.63236
|
4
|
1.880
|
8.69400 |
5 |
0.1990 |
3.73681 |
4
|
1.890
|
8.65700 |
5 |
0.2000 |
3.70000 |
2
|
1.900
|
8.70000 |
2 |
0.2110 |
3.96891 |
4
|
1.900 |
8.65400 |
3 |
0.2162 |
4.08496 |
4 |
1.900 |
8.63400 |
5 |
0.2278 |
4.28224 |
4
|
1.910
|
8.63500 |
3 |
0.2329 |
4.38669 |
4
|
1.910
|
8.61600
|
5 |
0.2445 |
4.60718 |
4
|
1.915 |
8.61100 |
5 |
0.2495
|
4.71163
|
4
|
1.920
|
8.62600 |
3 |
0.2611 |
4.92052 |
4 |
1.920 |
8.61000 |
5 |
0.2776 |
5.23385 |
4 |
1.925 |
8.60600 |
5 |
0.2825
|
5.32669
|
4
|
1.930 |
8.62600 |
3 |
0.2938
|
5.52398
|
4
|
1.930
|
8.60600
|
5 |
0.2988 |
5.62842 |
4 |
1.935 |
8.63000 |
3 |
0.3000 |
5.57000
|
1 |
1.935 |
8.61200
|
5 |
0.3000 |
5.65000 |
2
|
1.940
|
8.63000 |
3 |
0.4000
|
7.40000
|
2
|
1.940
|
8.60900 |
5 |
0.4036
|
7.63609
|
4
|
1.950
|
8.65000 |
3 |
0.4082
|
7.71732 |
4 |
1.950
|
8.63300 |
5 |
0.4187 |
7.91461 |
4
|
1.960
|
8.68300
|
3 |
0.4232
|
7.99584
|
4
|
1.960 |
8.67200 |
5 |
0.4355 |
8.18152 |
4 |
1.970
|
8.69500 |
5 |
0.4498
|
8.37881
|
4 |
2.000 |
8.95000
|
2 |
0.4643 |
8.64572 |
4
|
2.100
|
10.0000
|
2 |
0.4785
|
8.86622
|
4
|
2.200
|
11.6500 |
2 |
0.4926
|
9.10992 |
4
|
2.300 |
13.5500 |
2 |
0.5000 |
9.15000 |
2 |
2.400
|
15.5000
|
2 |
0.5605 |
10.1544
|
4 |
2.500
|
16.4500 |
2 |
0.6000 |
10.7500 |
2 |
2.600
|
17.0000
|
2 |
0.6243
|
11.0015 |
4 |
2.700 |
17.3000 |
2 |
0.6965
|
11.8023
|
4
|
2.800
|
17.5000
|
2 |
0.7000 |
11.7500 |
2
|
2.900
|
17.7000 |
2 |
0.7649
|
12.4173 |
4
|
3.000
|
17.8500 |
2 |
0.8000 |
12.7200 |
1 |
3.100
|
18.0000 |
2 |
0.8000 |
12.6500 |
2 |
3.200 |
18.1500 |
2 |
0.8300 |
12.8815 |
4 |
3.300 |
18.3000 |
2 |
0.8925 |
13.2297 |
4 |
3.400
|
18.3500 |
2 |
0.9000
|
13.1500 |
2 |
3.500
|
18.4000 |
2 |
1.000 |
13.5500 |
2 |
3.600 |
18.4500 |
2 |
Figure 13.1. Energy E in degrees
Kelvin of elementary excitations in helium II as a function of wave number
Q in reciprocal ?ngstroms(Ref.12).
Table
13.2. Knots and coefficients for the spline fit of the dispersion curve
of liquid 4He.
Knots |
Coefficients |
K(
1) = 0.0894 |
C(
1) =1.53895 |
K(
2) = 0.0894 |
C(
2) = 1.932 |
K(
3) = 0.0894 |
C(
3) = 4.8 |
K(
4) = 0.0894 |
C(
4) = 14.85 |
K(
5) = 0.15 |
C(
5) = 14.88 |
K(
6) = 0.510 |
C(
6) = 5.9384 |
K(
7) = 1.60 |
C(
7) = 16.5014 |
K(
8) = 2.023 |
C( 8) = 17.72455 |
K(
9) = 2.42 |
C(
9) = 18.43656 |
K(10)
= 2.665 |
C(10)
= 18.43545 |
K(11)
= 3.60 |
|
K(12)
= 3.60 |
|
K(13)
= 3.60 |
|
K(14)
= 3.60 |
|
Figure 13.2. Group velocity
of elementary excitations in helium II as a function of wave number Q
in reciprocal ?ngstroms (Ref.12).
Table
13.3. Recommended values of the dispersion curve of elementary excitations
in liquid 4He as a function of wavenumber Q.
Q (Å-1) |
E/k (K) |
Q (Å-1) |
E/k (K) |
0.00 |
0.00* |
1.85
|
8.866 |
0.05
|
0.804
|
1.90
|
8.667 |
0.10
|
1.747
|
1.95
|
8.644 |
0.15 |
2.757 |
2.00 |
8.833 |
0.20
|
3.772 |
2.05 |
9.271 |
0.25 |
4.772 |
2.10
|
9.941 |
0.30
|
5.749
|
2.15
|
10.784 |
0.35 |
6.694 |
2.20
|
11.742 |
0.40 |
7.598 |
2.25 |
12.751 |
0.45
|
8.452 |
2.30 |
13.753 |
0.50
|
9.249 |
2.35
|
14.687 |
0.55
|
9.979
|
2.40
|
15.492 |
0.60
|
10.641 |
2.45 |
16.111 |
0.65
|
11.237
|
2.50
|
16.544 |
0.70
|
11.767
|
2.55 |
16.832 |
0.75 |
12.232
|
2.60
|
17.019 |
0.80
|
12.633
|
2.65
|
17.147 |
0.85
|
12.971 |
2.70 |
17.258 |
0.90 |
13.248 |
2.75
|
17.366 |
0.95 |
13.464 |
2.80 |
17.471 |
1.00 |
13.62 |
2.85 |
17.573 |
1.05
|
13.717
|
2.90
|
17.671 |
1.10
|
13.757 |
2.95
|
17.765 |
1.15
|
13.74 |
3.00 |
17.855 |
1.20 |
13.667 |
3.05
|
17.94 |
1.25
|
13.54
|
3.10
|
18.019 |
1.30
|
13.359
|
3.15 |
18.093 |
1.35
|
13.125 |
3.20
|
18.161 |
1.40
|
12.839
|
3.25
|
18.222 |
1.45
|
12.503
|
3.30
|
18.276 |
1.50 |
12.118 |
3.35
|
18.323 |
1.55
|
11.684
|
3.40
|
18.363 |
1.60
|
11.202 |
3.45 |
18.394 |
1.65 |
10.68 |
3.50 |
18.417 |
1.70
|
10.148
|
3.55
|
18.431 |
1.75
|
9.644 |
3.60 |
18.435 |
1.80
|
9.204 |
|
|
* The
dispersion curve must be zero at zero wavenumber. Our spline returns
-2.485941E-4 K, which is incorrect, but negligible.
Figure 13.3. The fractional
deviation of values of the adopted database from the recommended values
for the dispersion curve for liquid 4He, expressed in percent.
Chronological Bibliography for Mutual Friction
1 |
.P. J. Bendt, R. D. Cowan, and J. L. Yarnell, "Excitations in Liquid
Helium: Thermodynamic Calculations," Phys. Rev. 113, 1386-1395 (1959). |
2 |
J.
L. Yarnell, G. P. Arnold, P. J. Bendt, and E. C. Kerr, “Excitations
in Liquid Helium: Neutron Scattering Measurements,” Phys. Rev.
113, 1379-1385 (1959). |
3 |
R.
A. Cowley and A. D. B. Woods, “Inelastic Scattering of Thermal
Neutrons from Liquid Helium,” Can. J. Phys. 49, 177-200 (1971). |
4 |
O.
W. Dietrich, E. H. Graf, C. H. Huang, and L. Passell, “Neutron
Scattering by Rotons in Liquid Helium,” Phys. Rev. A 5, 1377-1391
(1972). |
5 |
E.
C. Svensson, P. Martel, V. F. Sears, and A. D. B. Woods, “Neutron
Scattering Studies of the Dynamic Structure of Liquid 4He,”
Can. J. Phys. 54, 2178-2192 (1976). |
6 |
H.
Maris, “Phonon-Phonon Interactions in Liquid Helium,”
Rev. Mod. Phys. 49, 341-359 (1977). |
7 |
A.
D. B. Woods, P. A. Hilton, R. Scherm, and W. G. Stirling, “A
New Determination of the Roton Energy in Superfluid Liquid Helium,”
J. Phys. C 10, 145-149 (1977). |
8 |
D.
S. Greywall, “Specific Heat and Phonon Dispersion Curve of Liquid
4He,” Phys. Rev B 18, 2127-214 (1978). |
9 |
W.
G. Stirling, J. R. D. Copley, and P. A. Hilton, “High Resolution
Study of the Phonon Dispersion at Small Wave Vectors in Superfluid
4He,” in IAEA Symposium, Neutron Inelastic Scattering
(Vienna, 1978), Vol. III, pp. 45-52. |
10 |
E.
C. Svensson, R. Scherm, and A. D. B. Woods, “Temperature Dependence
of Phonons in Liquid Helium,” J. Phys. C 39, 211-214 (1978). |
11 |
J.
A. Tarvin and L. Passell, “Analysis of Line Shapes Observed
in the Scattering of Thermal Neutrons from Superfluid 4He,”
Phys. Rev. B 19, 1458-1462 (1979). |
12 |
R.
J. Donnelly, J. A. Donnelly, and R. N. Hills, “Specific Heat
and Dispersion Curve for Helium II,” J. Low Temp. Phys. 44,
471-489 (1981). |
13 |
W.
G. Stirling, “New High-Resolution Neutron Scattering Investigations
of Excitations in Liquid 4He,” presented at the Second
International Conference on Phonon Physics (unpublished) |
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