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《中国物理C》(英文)编辑部
2024年10月30日

THE PROBLEM OF THE COSMOLOGICAL CONSTANT

  • The cosmological term is necessaritly vanishing in a conformal gravitational theory, and the sum of the induced cosmological constants of all the brocken gauge symmetries cancels the curvature of the background spacetime. Thus the sum of all the cosmological constants is vanishing when the background spacetime is Minkowskian. Furthermore, the spontaneous breaking of a gauge symmetry through the Higgs mechanism is always accompanied by a phase transition of the background spacetime.
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  • [1] A. Einstein, Annal der Phys., 49(1916), 799; A. Einstein, Sitz. Phys.Akad. Wiss., 142(1917).[2] Ya. B. Zel'dovich, Usp. Fiz. Nauk.95(1968), 209.[3] J. Ellis, A. B. Lahanas, D. V. Nanopoulos and K. Tamvakis, Phys.Lett., 134B(1984), 429; J. Ellis,C.Kounnas and D. V. Nanopoulos, Nucl. Phys., B247(1984), 273; A. Srrominger and V. P. Nair, Phys.Rev.,D30(1984). 2528; E. Cremmer,B, Julia, J. Scherk, s. Ferrara, L. Cirardelln and P. van Nieuwen huizen, Nucl, Phys, B147(1979),105;L. E.Abbott, Phys. Leu.,150B(1985),427;W. Hiscock, Phys, Lett. 166B(1986),285;I.Ya.Arefeva, B. G. Dragovic and I. V. Volovich, Phys, Lett., 177B(1986),357;M. B. Green, Preprint QMC-85-15.[4] C.-Z. Zha, Phys. Lett.,171B(1986), 366.[5] I. Antoniadis, J. Iliopoulos and T. N. Tomaras, Nucl. Phys., B261(1985), 157[6] F. Del Aguila and G. D. Coughlan, Phys. Lett., 180B(1986), 25.[7] M. Carmeli, Classical Field (Whey-lnterscience Publication, USA, 1982)[8] E. S. Fradkin and A. A. Tseytlin, Phys. Rep, 119(1985), 233.
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Get Citation
ZHA Chao-Zheng. THE PROBLEM OF THE COSMOLOGICAL CONSTANT[J]. Chinese Physics C, 1987, 11(5): 699-703.
ZHA Chao-Zheng. THE PROBLEM OF THE COSMOLOGICAL CONSTANT[J]. Chinese Physics C, 1987, 11(5): 699-703. shu
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Received: 1900-01-01
Revised: 1900-01-01
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THE PROBLEM OF THE COSMOLOGICAL CONSTANT

    Corresponding author: ZHA Chao-Zheng,
  • Xinjiang University, Wulumuqi

Abstract: The cosmological term is necessaritly vanishing in a conformal gravitational theory, and the sum of the induced cosmological constants of all the brocken gauge symmetries cancels the curvature of the background spacetime. Thus the sum of all the cosmological constants is vanishing when the background spacetime is Minkowskian. Furthermore, the spontaneous breaking of a gauge symmetry through the Higgs mechanism is always accompanied by a phase transition of the background spacetime.

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