Unified Model of Electric Monopole and Magnetic Monopole

TANG JuFei

Chinese Physics C> 2000, Vol. 24> Issue(8) : 702-710

Unified Model of Electric Monopole and Magnetic Monopole

TANG JuFei ^,

Graduate School of Chinese Academy of Sciences,Beijing 100039,China

Abstract
HTML
Reference
Related

PDF

Abstract：
It is shown that the magnetic monopole and the electric monopole can be generated on an unified model based on the Hopf bundle (S³=S²×S¹) with the structure group U(1). The connection on the base manifold S² is divided into two types,the type of electric monopole and the type of magnetic monopole. The magnetic charge obeys the quantized condition,and the electric monopole is the solution where the magnetic quantum number n=0. The electric monopole and the magnetic monopole have the theoretical identity. They are two different states of one physical object. The time coordinate is introduced by the homotopic shift,and the electric monopole appears in an active model in the Minkowski space. The theory is Lorentz invariant.

References

[1]

. Dirac P A M .Proc.Roy .Soc.,1931,A133 :602. WU .T T ,YANG C N .Physical Review ,1975,D12 :384 5 3. Andrzej Trautman.International Journal of Theoretical Physics,1977,16( 8) :561— 565 4. Hopf H .Mathematische Annlen ,1931,10 4 :6375. Ryder L H .J.Phys.A :Math .Gen .,1980 ,13 :437— 447;Masatsugu Minami.Prog.of Theor .Phys.,1979,62 ( 4 ) 6. JIANG ZeHan .Introduction to Topology .Shanghai:Shanghai Press of Sciences and Technology(in Chinese) ,1978,66—69(江泽涵 .拓扑学引论 .上海 :上海科学技术出版社 ,1978,66— 69)

[1]	LIANG Jun , MA Zhong-Yu . Giant Monopole Resonance and Symmetry Energy. Chinese Physics C, 2007, 31(5): 470-474.
[2]	JIA Duojie , LI Xi-Guo . Monopole Dynamics of Yang-Mills Theory without Gauge-Fixing. Chinese Physics C, 2003, 27(4): 293-298.
[3]	Shen Yuelin , Ni Guangjiong . Berry's Connection and Wu-Yang's Monopole Potential. Chinese Physics C, 1995, 19(6): 500-507.
[4]	Cao Zhen , Ding Linkai . Chou-Yang Model for the Description of Ultrahigh Energy Soft Hadronic Interactions. Chinese Physics C, 1994, 18(11): 990-995.
[5]	FAN Xiao-Ling , ZHANG Chun-Sheng . A Parametrization Model of Hadron-Hadron Nuclear Interaction. Chinese Physics C, 1992, 16(2): 97-104.
[6]	QI Yong-Chang . ON THE SUPERHEAVY FERMION——SO(10) MONOPOLE ZERO-ENERGY BOUND STATES. Chinese Physics C, 1986, 10(5): 545-552.
[7]	YAN Jun-Hu . EXACT SOLUTION OF THE PAULI EQUATION IN THE FIELD OF A 'T HOOFT-POLYAKOV MONOPOLE. Chinese Physics C, 1985, 9(3): 367-370.
[8]	LI He-Nian , YUAN Yu-Kui , QIN Ke-Yu , ZHU Qing-Qi , WU Shi-Pei , LI Yan-Guo , ZHENG Rong-Ting , HUO An-Xiang . CHARGED HADRONIC MOMENTUM SPECTRA IN THE RANGE (5—50)GeV/c AT MOUNTAIN ALTITUDE. Chinese Physics C, 1985, 9(3): 268-272.
[9]	JIANG Xiang-Dong , ZHOU Xian-Jian . SO(10)×SO(8) MODEL WITH FRACTIONAL CHARGES, MONOPOLES AND PECULIAR PHOTONS. Chinese Physics C, 1985, 9(4): 421-429.
[10]	LI Bing-An , SHEN Qi-Xing , YU Hong . ELECTROWEAK INTERFERENCE EFFECTS IN THE HIGH ENERGY e⁺+e^－→e⁺+e^－+ HADRONS PROCESSES. Chinese Physics C, 1984, 8(1): 39-44.
[11]	XU De-Zhi . A STRUCTURE MODEL OF STRATONS AND LEPTONS. Chinese Physics C, 1983, 7(5): 546-549.
[12]	YIN PENG-CHENG , ZHOU GU-SHENG , WANG JIA-ZHU , WANG ZI . GLUE BAG MODEL AND MASS SPECTRA OF HADRONS. Chinese Physics C, 1981, 5(4): 417-428.
[13]	HUANG CHAO-SHANG , DAI YUAN-BEN . ANOMALOUS MAGNETIC MOMENT IN COMPOSITE MODEL OF LEPTONS. Chinese Physics C, 1981, 5(6): 699-705.
[14]	YIN LO , LI YANG-GUO , LIU XIAN-HUI . OPERATOR THEORY OF HADRON SCATTERING IN GEOMETRICAL MODEL. Chinese Physics C, 1981, 5(6): 653-663.
[15]	WANG MING-ZHONG , ZHENG XI-TE , XIAN DING-CHANG , ZHANG ZHENG-GANG , . A DISCUSSION ON THE MASS OF MONOPOLE. Chinese Physics C, 1981, 5(6): 741-743.
[16]	ZHU WEI , ZHANG MIN-SHENG , LU JI-ZONG , FENG CHENG-TIAN , CHU JUN-HAO . A φ⁴-TYPE BAG MODEL OF HADRONS——THE “RUBBER BAG”MODEL Ⅱ.THE MASS SPECTRA OF HADRONS. Chinese Physics C, 1979, 3(3): 266-271.
[17]	XU CHUN-XIAN , HUO AN-XIANG , YUAN YN-KUI , GU YI-DONG , LI TI-PEI , SHEN PEI-RO , JIA GUEI-BIN , XIAO QIAN-YI , ZHANG CHENG-MO , CHEN DUAN-BAO . THE NEGATIVE-POSITIVE RATIO OF CHARGED COSMIC RAY HADRONS AT THE 3220 m ABOVE SEA-LEVEL. Chinese Physics C, 1978, 2(5): 423-427.
[18]	WANG KE-LIN , HSIEN TING-CHANG , CHENG HSI-THE . ON THE MAGNETIC MONOPOLE AND DIPOLE SOLUTION OF THE SU(N) GAUGE FIELD THEORY IN A CURVED SPACE. Chinese Physics C, 1978, 2(3): 275-279.
[19]	TZU TUNG-PEI . THE NON-SINGULAR VECTOR POTENTIAL OF A MAGNETIC MONOPOLE IN THE DIRECTION OF MERIDIAN. Chinese Physics C, 1978, 2(1): 93-96.
[20]	LEE TZE-PING . ON CLASSICAL ANGULAR MOMENTUM OF AN ELECTRON-MAGNETIC MONOPOLE. Chinese Physics C, 1978, 2(4): 378-381.

Access

Get Citation

TANG JuFei. Unified Model of Electric Monopole and Magnetic Monopole[J]. Chinese Physics C, 2000, 24(8): 702-710.

TANG JuFei. Unified Model of Electric Monopole and Magnetic Monopole[J]. Chinese Physics C, 2000, 24(8): 702-710. shu

RIS(for EndNote,Reference Manager,ProCite)

BibTex

Txt

Milestone

Received: 1999-07-19
Revised: 1900-01-01

Article Metric

Article Views(2983)
PDF Downloads(554)
Cited by(0)

Policy on re-use

To reuse of subscription content published by CPC, the users need to request permission from CPC, unless the content was published under an Open Access license which automatically permits that type of reuse.

通讯作者: 陈斌, bchen63@163.com

1.
沈阳化工大学材料科学与工程学院沈阳 110142

Unified Model of Electric Monopole and Magnetic Monopole

TANG JuFei ^,

Corresponding author: TANG JuFei,

Graduate School of Chinese Academy of Sciences,Beijing 100039,China

Received Date: 1999-07-19
Accepted Date: 1900-01-01
Available Online: 2000-08-05

Abstract: It is shown that the magnetic monopole and the electric monopole can be generated on an unified model based on the Hopf bundle (S³=S²×S¹) with the structure group U(1). The connection on the base manifold S² is divided into two types,the type of electric monopole and the type of magnetic monopole. The magnetic charge obeys the quantized condition,and the electric monopole is the solution where the magnetic quantum number n=0. The electric monopole and the magnetic monopole have the theoretical identity. They are two different states of one physical object. The time coordinate is introduced by the homotopic shift,and the electric monopole appears in an active model in the Minkowski space. The theory is Lorentz invariant.