ライフサイエンスコーパス: liquid helium

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1 es in their three-dimensional environment of liquid helium.

2 alized in superconductors, atomic gases, and liquid helium.

3 result of unique cluster growth processes in liquid helium.

4 magnitude larger than those observed in bulk liquid helium.

5 operties that are different from the quantum liquids helium-3 and helium-4.

6 of a R- roton (a particle-like excitation in liquid helium-4) is antiparallel to its velocity.

7 quantum liquids -- such as superconductors, liquid helium and atom Bose-Einstein condensates -- that

8 c spins spontaneously align in a magnet, and liquid helium becomes superfluid.

9 specially in the case of liquid nitrogen- or liquid helium-cooled detectors) should be monitored.

10 mplexity, cost, and technical demands of the liquid-helium-cooled superconducting instruments require

11 Reported here is a study of the effects of liquid helium cooling on the fragmentation of ions forme

12 ly on the design and construction of a novel liquid helium cryostat that accommodates variable-sized

13 compressibility measurements on electrons on liquid helium demonstrating the formation of an incompre

14 haracterized in the gas phase, was formed in liquid helium droplets and studied with infrared spectro

15 and that the rapid quenching provided by the liquid helium inhibits its rearrangement to the more sta

16 When liquid helium is cooled to below its phase transition at

17 enic levels above a micrometer-thick film of liquid helium, is proposed as an easily manipulated stro

18 bility behavior when temperature crosses the liquid helium lambda point.

19 he top plate is cooled by heat exchange with liquid helium maintained at 4.2 K.

20 e and cytosine) are cooled to 0.37 kelvin in liquid helium nanodroplets and oriented in a large dc el

21 In superfluids, such as liquid helium or ultracold gases, the corresponding quan

22 via laser-excited Shpol'skii spectrometry at liquid helium temperature (4.2 K) is reported.

23 iority pollutants are directly determined at liquid helium temperature (4.2 K) with the aid of a cryo

24 sibility field H*(T)-is approximately 7 T at liquid helium temperature (4.2 K), significantly lower t

25 ifferent U isotopes ((238)U and (233)U), and liquid helium temperature time-resolved laser-induced fl

26 LLS is populated by thermal equilibration at liquid helium temperature.

27 ction at cryogenic temperatures (possibly at liquid helium temperatures and certainly above 75 K) imp

28 EPR spectra at liquid helium temperatures and MCD spectra at room tempe

29 e(3+) signal is abolished by illumination at liquid helium temperatures and one whose Fe(3+) signal i

30 is quantum yield is temperature invariant at liquid helium temperatures and shows a rather large kine

31 uantized modes of a quantum point contact at liquid helium temperatures to be imaged.

32 ear double resonance (ENDOR) spectroscopy at liquid helium temperatures, the Cu(II) coordination geom

33 ly attractive for high-field applications at liquid helium temperatures.

34 (-1) and 10(4) cm(2) V(-1) s(-1) at room and liquid-helium temperatures, respectively, allowing the o

35 , however, the QHE has been observed only at liquid-helium temperatures.

36 olid-phase compounds Cu(hfac)(2)L(R) at low (liquid helium) temperatures and approaches developed for

37 emingly remote physical systems ranging from liquid helium, ultracold atoms and superconducting thin

38 asts with previous experiments on superfluid liquid helium where hysteresis was observed directly in

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