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Impurity scattering in superfluid he...
~
Baumgardner, James Edward, II.
Impurity scattering in superfluid helium-3: A new phase.
紀錄類型:
書目-電子資源 : Monograph/item
正題名/作者:
Impurity scattering in superfluid helium-3: A new phase.
作者:
Baumgardner, James Edward, II.
面頁冊數:
194 p.
附註:
Adviser: Douglas D. Osheroff.
附註:
Source: Dissertation Abstracts International, Volume: 65-11, Section: B, page: 5787.
Contained By:
Dissertation Abstracts International65-11B.
標題:
Physics, Condensed Matter.
電子資源:
http://pqdd.sinica.edu.tw/twdaoapp/servlet/advanced?query=3153091
ISBN:
9780496135370
Impurity scattering in superfluid helium-3: A new phase.
Baumgardner, James Edward, II.
Impurity scattering in superfluid helium-3: A new phase.
- 194 p.
Adviser: Douglas D. Osheroff.
Thesis (Ph.D.)--Stanford University, 2005.
Having thus established the initial temperatures of the A-B transition on warming and cooling, TAB,w and TAB,c respectively, we consider the value of the equilibrium thermodynamic transition temperature, TAB. We develop a method for determining this temperature from precise measurements of the maximum frequency shifts and susceptibilities of the A-like and B phases. We find that TAB is equal to TAB,w within experimental error for both samples at all pressures where this measurement is possible. On this basis, we present the first thermodynamic A-B phase diagram of superfluid 3He in aerogel. We find that this phase diagram is substantially modified from the bulk, in a manner that is density-independent. We show that for any equal spin pairing state with transverse frequency shifts that agree with the measured value of our A-like phases, the order parameter is uniquely determined from the slope of the equilibrium A-B phase diagram. We tentatively identify the A-like phase as being the planar (two-dimensional) state, which has never before been reported to exist.
ISBN: 9780496135370Subjects--Topical Terms:
226939
Physics, Condensed Matter.
Impurity scattering in superfluid helium-3: A new phase.
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Having thus established the initial temperatures of the A-B transition on warming and cooling, TAB,w and TAB,c respectively, we consider the value of the equilibrium thermodynamic transition temperature, TAB. We develop a method for determining this temperature from precise measurements of the maximum frequency shifts and susceptibilities of the A-like and B phases. We find that TAB is equal to TAB,w within experimental error for both samples at all pressures where this measurement is possible. On this basis, we present the first thermodynamic A-B phase diagram of superfluid 3He in aerogel. We find that this phase diagram is substantially modified from the bulk, in a manner that is density-independent. We show that for any equal spin pairing state with transverse frequency shifts that agree with the measured value of our A-like phases, the order parameter is uniquely determined from the slope of the equilibrium A-B phase diagram. We tentatively identify the A-like phase as being the planar (two-dimensional) state, which has never before been reported to exist.
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We present continuous-wave NMR measurements of superfluid 3He confined to two low-density silica aerogels, with porosities of 99.3% and 98.6%. we find a first-order transition on cooling between two superfluid phases, from an A-like equal-spin pairing phase to a B phase. Careful measurements of the NMR spectra, integrated susceptibility, and average frequency shift demonstrate a broadened first-order transition on warming, from the B phase to possibly another A-like equal-spin pairing phase. This A-B transition on warming occurs over a broad range of temperatures, and in both samples, it is unable to convert the entire sample from the B to A-like phase before reaching Tc,aero By performing "trajectory" measurements (warming from the B phase until the A-like phase is seen, then subsequently cooling), we are able to show that the A-like phases on warming and cooling are identical. Measurements of the gap suppression in the A-like phase show that the aerogel has a single value of Tc, so that the width of the A-B transition is caused not by inhomogeneous broadening of the superfluid transition, but rather by pinning of the A-B interface.
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