»ù±¾ÊÍÒå:

²£É« °®Òò˹̹ÆøÌå

ÍøÂçÊÍÒå

1)bose einstein gas,²£É« °®Òò˹̹ÆøÌå

2)Bose,²£É«

3)Boson peak,²£É«·å

4)bosonization,²£É«»¯

5)Bose integral,²£É«»ý·Ö

6)g-boson,g²£É«×Ó

7)Bose gas,²£É«ÆøÌå

8)boson,²£É«×Ó

9)Schwinger boson,Schwinger²£É«×Ó

10)Quasi-boson CLC O413.1,×¼²£É«×Ó

Ó÷¨ºÍÀý¾ä

From Quantum Theory to Bose-Einstein Statistics;

´ÓÁ¿×ÓÂÛµ½²£É«-°®Òò˹̹ͳ¼Æ

Moreover,chemical potentials are extremely important in deducing Bose-Einstein coacerva.

Ö÷Òª½éÉÜ»¯Ñ§ÊÆÔÚÈÈÁ¦Ñ§Í³¼ÆÎïÀíÖм¸¸ö֪ʶµã´¦µÄ¼ÆËãÓëÓ¦ÓÃ:ÓÃÈÈÁ¦Ñ§·½·¨¼ÆËãÀíÏëÆøÌåµÄ»¯Ñ§ÊÆ;ϵͳÏà±ä¹ý³ÌÖеĻ¯Ñ§ÊƲ¢ÓÉ´ËÍƵ¼¿ËÀ­çêÁú·½³Ì;ÓÃͳ¼Æ·½·¨¼ÆËã×ñ´Ó²£¶ú×ÈÂüͳ¼ÆµÄÀíÏëÆøÌåµÄ»¯Ñ§ÊÆ;ÔÚ²£É«·Ö²¼ÖÐ,ÍƵ¼²£É«¡ª¡ª¡ª°®Òò˹̹Äý¾ÛÏÖÏóÖл¯Ñ§ÊƵÄÓ¦ÓÃ;ÔÚ·ÑÃ×·Ö²¼ÖÐ,¼ÆËã·ÑÃ×µç×ÓµÄÐÔÖÊ,µç×ӵĻ¯Ñ§ÊÆÆðµ½¾ö¶¨ÐÔµÄ×÷Óá£

The Boson peak of Pr~(3+), Lu~(3+)-doped 20GaF_3-15InF_3-20CdF_2-15ZnF_2-20PbF_2-10SnF_2 glasses was investigated by means of Raman spectrum and DSC.

½«À­Âü¹âÆ×ÓëÈÈ·ÖÎö·½·¨Ïà½áºÏ,Ñо¿ÁËÔÚ20GaF3 15InF3 20CdF2 15ZnF2 20PbF2 10SnF2²£Á§ÏµÍ³Öв£É«·åÓëÏ¡ÍÁÀë×ÓPr3+,Lu3+²ôÔÓŨ¶ÈµÄ¹Øϵ¡£

Chiral Bosonization of Superconformal Ghosts;

³¬¹²ÐÎ¹í³¡ÏµÍ³ÊÖÕ÷²£É«»¯

By using the bosonization approach and renormalization group analysis,we study the ground state phase diagram of one-dimensional extended Hubbard model at half-filling in the regime where U and V are both positive but less than t, finding that the system shows three distinct ground states characterized by the spin-density-wave,the charge-density-wave and the bond-charge-density-wave,respectively.

ÎÒÃÇÀûÓò£É«»¯ºÍÖØÕû»¯Èº·ÖÎöµÄ·½·¨Ñо¿ÁË°ëÂúÌî¿ÕÇÒÅųâÊÆСÓÚԾǨ¶¯ÄÜʱµÄһάÀ©Õ¹ºÕ²®ÌØÄ£Ð͵Ļù̬Ïàͼ,·¢ÏÖ»ù̬ÏàͼÊÇÓÉ×ÔÐýÃܶȲ¨,µçºÉÃܶȲ¨ºÍ¼üºÉÃܶȲ¨×é³É¡£

By using bosonization technique and Jordan-Wigner transformation,we study the spin(-1/2XY) model in external magnetic field.

²ÉÓÃJordan-W igner±ä»»ºÍ²£É«»¯·½·¨Ñо¿ÍⳡÖеÄ×ÔÐý-1/2XYÄ£ÐÍ¡£

Using the characteristics of Fermi integral and Bose integral and theory of thermodynamics, We discuss the characteristics of ideal quantum gas in a process of throttling expansion, and an analytical expression of Jouleª²Thomson coefficient (JTC) of ideal quantum gas is derived in this paper.

Ó¦Ó÷ÑÃ×»ý·ÖºÍ²£É«»ý·ÖµÄÌØÐÔÒÔ¼°ÈÈÁ¦Ñ§ÀíÂÛ,ÌÖÂÛÀíÏëÁ¿×ÓÆøÌåÔÚ½ÚÁ÷ÅòÕ͹ý³ÌÖеÄÌØÐÔ,µ¼µÃÀíÏëÁ¿×ÓÆøÌå½¹ÌÀϵÊýµÄ½âÎö±í´ïʽ,ÏêϸÌÖÂÛÁ˵ÍÎÂÏÂÁ¿×ÓÆøÌåµÄ¶¨Ñ¹ÈÈÈݺͽ¹ÌÀϵÊý,²ûÃ÷ÁËϵͳµÄÁ¿×Ó±¾ÐÔ¶Ô½¹ÌÀϵÊýµÄ¹±Ïס£

Using the fundamental equations of Bose systems, the characteristics of Bose integral and theory of thermodynamics, an analytical expression of Joule-Thomson coefficient (JTC) of ideal Bose gas is derived in this paper.

Ó¦Óò£É«ÏµÍ³µÄ»ù±¾·½³Ì ,²£É«»ý·ÖµÄÌØÐÔÒÔ¼°ÈÈÁ¦Ñ§ÀíÂÛ ,µ¼µÃÀíÏ벣ɫÆøÌå½¹ÌÀϵÊýµÄ½âÎö±í´ïʽ ,ÏêϸÌÖÂÛÁ˵ÍÎÂϲ£É«ÆøÌåµÄ¶¨Ñ¹ÈÈÈݺͽ¹ÌÀϵÊý ,²ûÃ÷ÁËϵͳµÄÁ¿×Ó±¾ÐÔ¶Ô½¹ÌÀϵÊýµÄ¹±Ï× ¡£

Thermodynamic properties of a weakly interacting Bose gas in a weak magnetic field;

Èõ´Å³¡ÖÐÈõÏ໥×÷Óò£É«ÆøÌåµÄÈÈÁ¦Ñ§ÐÔÖÊ

The influence of weak interaction on thermodynamic properties and the stability of imperfect Bose gas;

Ï໥×÷ÓöԲ£É«ÆøÌåÈÈÁ¦Ñ§ÐÔÖʼ°Îȶ¨ÐÔµÄÓ°Ïì

Vortex solution of weak interacting Bose gases;

ÈõÏ໥×÷Óò£É«ÆøÌåµÄÎÐÐý½â

The Unsaterated Pressure Law of Film System of Bosons;

²£É«×Ó±¡Ä¤ÏµÍ³µÄδ±¥ºÍÕôÆûѹ¶¨ÂÉ

The Formulas of the Coefficients of Fractional Parentage of Bosons(¢ò)---The explicit expressions of coefficients of fractional parentage of four bosons;

²£É«×ÓÇ×̬±ÈϵÊýµÄ¹«Ê½£¨¢ò£©©¤¡ªËIJ£É«×ÓÇ×̬±ÈϵÊýµÄÏÔʾʽ

Vortex solution in charge boson system;

ºÉµç²£É«×ÓϵͳµÄÎÐÐý½â

The thermodynamic properties in one-dimensional S=1 Heisenberg antiferromagnet with single-ion anisotropy in the presence of a transverse magnetic field is obtained on the basis of the Schwinger boson mean-field theory.

ÀûÓøĽøµÄSchwinger²£É«×Óƽ¾ù³¡ÀíÂÛ ,Ñо¿Á˺áÏòÍâ¼Ó´Å³¡ÏÂ×ÔÐýΪ 1µÄµ¥Á£×Ó¸÷ÏòÒìÐÔº£É­±¤·´Ìú´ÅÁ´µÄÈÈÁ¦Ñ§ÐÔÖÊ ¡£