For the TZ metric on the moduli
space <
span id="mml
si1" cla
ss="mathml
src"><
span cla
ss="formulatext
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science?_ob=MathURL&_method=retrieve&_eid=1-
s2.0-S0001870816301670&_mathId=
si1.gif&_u
ser=111111111&_pii=S0001870816301670&_rdoc=1&_i
ssn=00018708&md5=0ef4c0900e91c930d6acfbe98ebcc9b6" title="Click to view the MathML
source">M<
sub>0,n
sub>
span><
span cla
ss="mathContainer hidden"><
span cla
ss="mathCode">
span>
span>
span> of
n -pointed rational curve
s, we con
struct a Kähler potential in term
s of the Fourier coefficient
s of the Klein'
s Hauptmodul. We define the
space <
span id="mml
si2" cla
ss="mathml
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span cla
ss="formulatext
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science?_ob=MathURL&_method=retrieve&_eid=1-
s2.0-S0001870816301670&_mathId=
si2.gif&_u
ser=111111111&_pii=S0001870816301670&_rdoc=1&_i
ssn=00018708&md5=082ac70425503cfffe4f36b606c622a5" title="Click to view the MathML
source">S<
sub>g,n
sub>
span><
span cla
ss="mathContainer hidden"><
span cla
ss="mathCode">
span>
span>
span> a
s holomorphic fibration <
span id="mml
si3" cla
ss="mathml
src"><
span cla
ss="formulatext
stixSupport mathImg" data-mathURL="/
science?_ob=MathURL&_method=retrieve&_eid=1-
s2.0-S0001870816301670&_mathId=
si3.gif&_u
ser=111111111&_pii=S0001870816301670&_rdoc=1&_i
ssn=00018708&md5=cef116e0fcbc7c05f764baad31d315e4" title="Click to view the MathML
source">S<
sub>g,n
sub>→S<
sub>g
sub>
span><
span cla
ss="mathContainer hidden"><
span cla
ss="mathCode">
span>
span>
span> over the Schottky
space <
span id="mml
si4" cla
ss="mathml
src"><
span cla
ss="formulatext
stixSupport mathImg" data-mathURL="/
science?_ob=MathURL&_method=retrieve&_eid=1-
s2.0-S0001870816301670&_mathId=
si4.gif&_u
ser=111111111&_pii=S0001870816301670&_rdoc=1&_i
ssn=00018708&md5=d5a11d01b9b68b1dcc8800a492859b11" title="Click to view the MathML
source">S<
sub>g
sub>
span><
span cla
ss="mathContainer hidden"><
span cla
ss="mathCode">
span>
span>
span> of compact Riemann
surface
s of genu
s g, where the fiber
s are configuration
space
s of
n point
s. For the tautological line bundle
s <
span id="mml
si21" cla
ss="mathml
src"><
span cla
ss="formulatext
stixSupport mathImg" data-mathURL="/
science?_ob=MathURL&_method=retrieve&_eid=1-
s2.0-S0001870816301670&_mathId=
si21.gif&_u
ser=111111111&_pii=S0001870816301670&_rdoc=1&_i
ssn=00018708&md5=3d5f378089a3be2f660ec640afc7b993" title="Click to view the MathML
source">L<
sub>i
sub>
span><
span cla
ss="mathContainer hidden"><
span cla
ss="mathCode">
span>
span>
span> over <
span id="mml
si2" cla
ss="mathml
src"><
span cla
ss="formulatext
stixSupport mathImg" data-mathURL="/
science?_ob=MathURL&_method=retrieve&_eid=1-
s2.0-S0001870816301670&_mathId=
si2.gif&_u
ser=111111111&_pii=S0001870816301670&_rdoc=1&_i
ssn=00018708&md5=082ac70425503cfffe4f36b606c622a5" title="Click to view the MathML
source">S<
sub>g,n
sub>
span><
span cla
ss="mathContainer hidden"><
span cla
ss="mathCode">
span>
span>
span>, we define Hermitian metric
s <
span id="mml
si343" cla
ss="mathml
src"><
span cla
ss="formulatext
stixSupport mathImg" data-mathURL="/
science?_ob=MathURL&_method=retrieve&_eid=1-
s2.0-S0001870816301670&_mathId=
si343.gif&_u
ser=111111111&_pii=S0001870816301670&_rdoc=1&_i
ssn=00018708&md5=7512e6237c51f5e31429f4e8181c4cca" title="Click to view the MathML
source">h<
sub>i
sub>
span><
span cla
ss="mathContainer hidden"><
span cla
ss="mathCode">
span>
span>
span> in term
s of Fourier coefficient
s of a covering map
J of the Schottky domain. We define the regularized cla
ssical Liouville action
S and
show that <
span id="mml
si39" cla
ss="mathml
src"><
span cla
ss="formulatext
stixSupport mathImg" data-mathURL="/
science?_ob=MathURL&_method=retrieve&_eid=1-
s2.0-S0001870816301670&_mathId=
si39.gif&_u
ser=111111111&_pii=S0001870816301670&_rdoc=1&_i
ssn=00018708&md5=e25a109b45c6a842087c5a55780dd6e3" title="Click to view the MathML
source">exp{S/π}
span><
span cla
ss="mathContainer hidden"><
span cla
ss="mathCode">
span>
span>
span> i
s a Hermitian metric in the line bundle <
span id="mml
si9" cla
ss="mathml
src">
source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0001870816301670&_mathId=si9.gif&_user=111111111&_pii=S0001870816301670&_rdoc=1&_issn=00018708&md5=7bc83484836b060081b10fc5db7c461a">ss="imgLazyJSB inlineImage" height="16" width="93" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0001870816301670-si9.gif">script>style="vertical-align:bottom" width="93" alt="View the MathML source" title="View the MathML source" src="http://origin-ars.els-cdn.com/content/image/1-s2.0-S0001870816301670-si9.gif">script><
span cla
ss="mathContainer hidden"><
span cla
ss="mathCode">
span>
span>
span> over <
span id="mml
si2" cla
ss="mathml
src"><
span cla
ss="formulatext
stixSupport mathImg" data-mathURL="/
science?_ob=MathURL&_method=retrieve&_eid=1-
s2.0-S0001870816301670&_mathId=
si2.gif&_u
ser=111111111&_pii=S0001870816301670&_rdoc=1&_i
ssn=00018708&md5=082ac70425503cfffe4f36b606c622a5" title="Click to view the MathML
source">S<
sub>g,n
sub>
span><
span cla
ss="mathContainer hidden"><
span cla
ss="mathCode">
span>
span>
span>. We explicitly compute the Chern form
s of the
se Hermitian line bundle
sss="formula" id="fm0010">
We prove that a
smooth real-valued function <
span id="mml
si11" cla
ss="mathml
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source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0001870816301670&_mathId=si11.gif&_user=111111111&_pii=S0001870816301670&_rdoc=1&_issn=00018708&md5=b8b60a4d1ac037fb01da529eaba12c24">ss="imgLazyJSB inlineImage" height="18" width="186" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0001870816301670-si11.gif">script>style="vertical-align:bottom" width="186" alt="View the MathML source" title="View the MathML source" src="http://origin-ars.els-cdn.com/content/image/1-s2.0-S0001870816301670-si11.gif">script><
span cla
ss="mathContainer hidden"><
span cla
ss="mathCode">
span>
span>
span> on <
span id="mml
si2" cla
ss="mathml
src"><
span cla
ss="formulatext
stixSupport mathImg" data-mathURL="/
science?_ob=MathURL&_method=retrieve&_eid=1-
s2.0-S0001870816301670&_mathId=
si2.gif&_u
ser=111111111&_pii=S0001870816301670&_rdoc=1&_i
ssn=00018708&md5=082ac70425503cfffe4f36b606c622a5" title="Click to view the MathML
source">S<
sub>g,n
sub>
span><
span cla
ss="mathContainer hidden"><
span cla
ss="mathCode">
span>
span>
span>, a potential for thi
s special difference of WP and TZ metric
s, coincide
s with the renormalized hyperbolic volume of a corre
sponding Schottky 3-manifold. We extend the
se re
sult
s to the qua
si-Fuch
sian group
s of type <
span id="mml
si12" cla
ss="mathml
src"><
span cla
ss="formulatext
stixSupport mathImg" data-mathURL="/
science?_ob=MathURL&_method=retrieve&_eid=1-
s2.0-S0001870816301670&_mathId=
si12.gif&_u
ser=111111111&_pii=S0001870816301670&_rdoc=1&_i
ssn=00018708&md5=46bf961eaec02c7956e2adaee582d856" title="Click to view the MathML
source">(g,n)
span><
span cla
ss="mathContainer hidden"><
span cla
ss="mathCode">
span>
span>
span>.