참고문헌 (16)

1. Wiener Ber. II J Stefan 79 391 1879 Stefan, J.: Über die beziehung zwischen der wärmestrahlung und der temperatur. Wiener Ber. II 79, 391 (1879) 

2. Ann. der Phys. und Chemie. L Boltzmann 22 291 1884 10.1002/andp.18842580616 Boltzmann, L.: Ableitung des Stefan’schen Gesetzes, betreffend die Abhängigkeit der Wärmestrahlung von der Temperatur aus der electromagnetischen Lichttheorie. Ann. der Phys. und Chemie. 22, 291 (1884) 

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3. Ann. d. Phys. M Planck 4 553 1901 10.1002/andp.19013090310 Planck, M.: Über das gesetz der energieverteilung im normalspectrum. Ann. d. Phys. 4, 553 (1901) 

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4. Also known as the Stefan-Boltzmann law is the expression for the emitted power per unit area $${\cal P}(T)= {c \over 4} u(T) \equiv \sigma T^4$$ P ( T ) = c 4 u ( T ) ≡ σ T 4 where $$\sigma $$ σ is named the Stefan-Boltzmann constant 

5. Maxwell, JC.: A Treatise on Electricity and Magnetism. Oxford (1873) 

6. Planck, M.: Über irreversible strahlungsvorgänge, Sitz. der Preußischen Akademie der Wissenschaften, Berlin, 5, 440 (1899) 

7. Phys. Scr. T H Paul 165 014027 2015 10.1088/0031-8949/2015/T165/014027 Paul, H., Greenberger, D.M., Stenholm, S.T., Schleich, W.P.: Phys. Scr. T 165, 014027 (2015) 

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8. 10.1007/BF00670992 Such a generalization has also been discussed by J.A.S. de Lima and J. Santos, Int. J. Theor. Phys. 34, 127 (1995) in the context of general relativity 

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9. In quantum theory, these functions are known to be $$F(\alpha )= g_{{1+ \kappa }}(e^\alpha )=\text{Li}_{1+ \kappa }(e^\alpha ) $$ F ( α ) = g 1 + κ ( e α ) = Li 1 + κ ( e α ) for Bosons and $$F(\alpha )= f_{{1+ \kappa }}(e^\alpha )=-\text{ Li }_{1+ \kappa }(-e^\alpha ) $$ F ( α ) = f 1 + κ ( e α ) = - Li 1 + κ ( - e α ) for Fermions, where $$\text{ Li }_\nu (z)$$ Li ν ( z ) is the polylogarithm function 

10. Phys. Rev. Lett. V Romero-Rochín 94 130601 2005 10.1103/PhysRevLett.94.130601 Romero-Rochín, V.: Equation of state of an interacting Bose gas confined by a harmonic trap: the role of the harmonic pressure. Phys. Rev. Lett. 94, 130601 (2005) 

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11. Rao, S.: Weyl semi-metals: a short review, arXiv:1603.02821 

12. See for example Y. N. Srivastava, A. Widom and J. Swain , Thermodynamic Equations of State for Dirac and Majorana Fermions, arXiv:hep-ph/9709434 

13. New J. Phys. B Wunsch 10 103027 2008 10.1088/1367-2630/10/10/103027 Wunsch, B., Guinea, F., Sols, F.: Dirac-point engineering and topological phase transitions in honeycomb optical lattices. New J. Phys. 10, 103027 (2008) 

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14. Eur. Phys. J. B G Montambaux 72 509 2009 10.1140/epjb/e2009-00383-0 Montambaux, G., Piéchon, F., Fuchs, J.-N., Goerbig, M.O.: A universal Hamiltonian for the motion and the merging of Dirac cones in a two-dimensional crystal. Eur. Phys. J. B 72, 509 (2009) 

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15. Phys. Rev. Lett. S Banerjee 103 016402 2009 10.1103/PhysRevLett.103.016402 Banerjee, S., Singh, R.R., Pardo, V., Pickett, W.E.: Tight-binding modeling and low-energy behavior of the semi-dirac point. Phys. Rev. Lett. 103, 016402 (2009) 

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16. C Pethick 2002 Bose-Einstein Condensation in Dilute Gases Pethick, C., Smith, H.: Bose-Einstein Condensation in Dilute Gases. Cambridge University Press, Cambridge (2002) 

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