QT n -(4) L At the low temperature end, T = 4.2 K and (5) and the parameters p, A, X, Cp are constant and over a short length near the end the temperature variation can be taken as linear, which means that d2T -0 dx 2 From (3), (4), and (5) LI2pX 1 QT-Cp QL By differentiating dQT LI2 pX 1 dQL Cp Q~
✦ LIBER ✦
What is the physics behind the3He–4He anomaly?
✍ Scribed by W. Neubert; A.S. Botvina
- Publisher
- Springer
- Year
- 2000
- Tongue
- English
- Weight
- 188 KB
- Volume
- 7
- Category
- Article
- ISSN
- 1434-601X
No coin nor oath required. For personal study only.
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