Built on

E. Witten, “Noncommutative Geometry and String Field Theory,” Nucl.Phys
1986
Earlier work this paper cites.
R. C. Myers, S. Penati, M. Pernici, and A. Strominger, “SOFT DILATON THEOREM IN COVARIANT STRING FIELD THEORY,” Nucl.Phys
1988
Earlier work this paper cites.
B. Zwiebach, “Interpolating string field theories,” Mod.Phys.Lett
1992
Earlier work this paper cites.
P. Fendley, F. Lesage, and H. Saleur, “Solving 1-d plasmas and 2-d boundary problems using Jack polynomials and functional relations,” J.Statist.Phys
1995
Earlier work this paper cites.
A. Hashimoto and N. Itzhaki, “Observables of string field theory,” JHEP
2002
Earlier work this paper cites.
D. Gaiotto, L. Rastelli, A. Sen, and B. Zwiebach, “Ghost structure and closed strings in vacuum string field theory,” Adv.Theor.Math.Phys
2003
Earlier work this paper cites.
M. Schnabl, “Analytic solution for tachyon condensation in open string field theory,” Adv.Theor.Math.Phys
2006
Earlier work this paper cites.
Y. Okawa, “Comments on Schnabl’s analytic solution for tachyon condensation in Witten’s open string field theory,” JHEP
2006
Earlier work this paper cites.

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Then

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2011
Later among the works it cites.
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2012

Energy from the gauge invariant observables

Baba, Takayuki, Ishibashi, Nobuyuki

Understand

For a classical solution |Psi> in Witten's cubic string field theory, the gauge invariant observable <I|V|Psi> is conjectured to be equal to the difference of the one-point functions of the closed string state corresponding to V, between the trivial vacuum and the one described by |Psi>.

For a static solution |Psi>, if V is taken to be the graviton vertex operator with vanishing momentum, the gauge invariant observable is expected to be proportional to the energy of |Psi>.
We prove this relation assuming that |Psi> satisfies equation of motion and some regularity conditions.
We discuss how this relation can be applied to various solutions obtained recently.

Built on

E. Witten, “Noncommutative Geometry and String Field Theory,” Nucl.Phys
1986
Earlier work this paper cites.
R. C. Myers, S. Penati, M. Pernici, and A. Strominger, “SOFT DILATON THEOREM IN COVARIANT STRING FIELD THEORY,” Nucl.Phys
1988
Earlier work this paper cites.
B. Zwiebach, “Interpolating string field theories,” Mod.Phys.Lett
1992
Earlier work this paper cites.
P. Fendley, F. Lesage, and H. Saleur, “Solving 1-d plasmas and 2-d boundary problems using Jack polynomials and functional relations,” J.Statist.Phys
1995
Earlier work this paper cites.
A. Hashimoto and N. Itzhaki, “Observables of string field theory,” JHEP
2002
Earlier work this paper cites.
D. Gaiotto, L. Rastelli, A. Sen, and B. Zwiebach, “Ghost structure and closed strings in vacuum string field theory,” Adv.Theor.Math.Phys
2003
Earlier work this paper cites.
M. Schnabl, “Analytic solution for tachyon condensation in open string field theory,” Adv.Theor.Math.Phys
2006
Earlier work this paper cites.
Y. Okawa, “Comments on Schnabl’s analytic solution for tachyon condensation in Witten’s open string field theory,” JHEP
2006
Earlier work this paper cites.