{"arxiv_id":"hep-ph/9305348","incoming":{"papers":10,"sentences":12,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":1,"sentences":2,"quotes":[{"arxiv_id":"2211.06211","title":"$K_0^\\ast(1430)$ Twist-2 Distribution Amplitude and $B_s,D_s \\to K_0^\\ast(1430)$ Transition Form Factors","url":"/paper/2211.06211","section":"$B_s,D_s→K_0^∗$ TFFs within LCSRs","sentence":"Substituting Eq. [ref] into Eq. [ref], one can get [equation] On the other hand, the invariant amplitude after Borel transformation can also be written as [ref] [equation] Finally, equating Eqs. [ref] with [ref], the LCSR of TFF $f_+(q^2)$ can be obtained as [equation] Similarly, [equation] with [equation] In particular, the upper limit of the integral of variable $u$ in LCSRs [ref], [ref] and [ref] is $u_0$ instead of 1, because the lower limit of the integral variable $s$ in the dispersion relationship [ref], $t_min$, is larger than, but not equal to, $m_Q^2$.","intent_p":0.94,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":5,"sentences":5,"quotes":[{"arxiv_id":"2512.11741","title":"Determination of $B$-meson distribution amplitudes from $B\\to \\pi,K,D$ transition form factors","url":"/paper/2512.11741","section":"B to pseudoscalar Meson Form Factors from Light-Cone Sum Rules","sentence":"In the early stage, the LCSR approach was formulated using an $B$-meson interpolating current together with the light meson LCDAs [ref] .","intent_p":0.95,"contests_p":null},{"arxiv_id":"0804.3198","title":"$B \\to K_1 \\gamma$ Decays in the Light-Cone QCD Sum Rules","url":"/paper/0804.3198","section":"Introduction","sentence":"The method of LC sum rules has been widely used in the studies of nonperturbative processes, including weak baryon decays [ref] , heavy meson decays [ref] , and heavy to light transition form factors [ref] .","intent_p":0.91,"contests_p":null},{"arxiv_id":"2112.12674","title":"$B\\to D \\ell \\nu_\\ell$ form factors beyond leading power and extraction of $|V_{cb}|$ and $R(D)$","url":"/paper/2112.12674","section":"Introduction","sentence":"This machinery can be formulated both in the context of QCD as well as in soft-collinear effective theory (SCET), as pioneered in the work of [ref] and [ref] , respectively.","intent_p":0.83,"contests_p":null},{"arxiv_id":"0807.1171","title":"Form Factors of $B_{u,d,s}$ Decays into P-Wave Axial-Vector Mesons in the Light-Cone Sum Rule Approach","url":"/paper/0807.1171","section":"Introduction","sentence":"The method of light-cone sum rules has been widely used in the studies of nonperturbative processes, including weak baryon decays [ref] , heavy meson decays [ref] , and heavy to light transition form factors [ref] .","intent_p":0.92,"contests_p":null},{"arxiv_id":"2206.05631","title":"Borel-Laplace Sum Rules with $\\tau$ decay data, using OPE with improved anomalous dimensions","url":"/paper/2206.05631","section":"Final results and conclusions","sentence":"LCSRs involve partial resummations in the three-point QCD sum rules and can be used to evaluate form factors and other hadronic quantities (cf. Refs. [ref] for some earlier works on the subject).","intent_p":0.98,"contests_p":null}]}],"unlabelled_sentences":5},"outgoing":{"papers":0,"sentences":0,"groups":[],"unlabelled_sentences":0},"claims":[],"thresholds":{"intent_p":0.8,"supports_p":0.95,"contests_p":0.7},"method":"Citing sentences come from each paper's LaTeX source; every \\cite marks the sentence and the works it cites. Pith's classifier typed each sentence. A label is shown at intent probability 0.8 or more (0.95 for support), a contest at 0.7 or more. Measured accuracy against two blind model families is at https://pith.science/accuracy. The quoted sentences are the citing authors' own.","held_up":null,"_links":{"html":"https://pith.science/paper/hep-ph/9305348"}}