{"arxiv_id":"hep-th/9904207","incoming":{"papers":74,"sentences":106,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":2,"sentences":2,"quotes":[{"arxiv_id":"2409.06454","title":"Kerr Black hole mimickers sourced by a string fluid","url":"/paper/2409.06454","section":"Lagrangian and equations of motion","sentence":"To arrive at this action, we followed the analysis of GHY [ref] (also, [ref] ), whose own starting point was Sen's effective action for the final state of the decay of unstable $D$-branes at the end of tachyon condensation and near the minimum of the tachyon potential where it vanishes [ref] .","intent_p":0.81,"contests_p":null},{"arxiv_id":"1911.11780","title":"Topological Superconductors on Superstring Worldsheets","url":"/paper/1911.11780","section":"Vacuum manifolds of tachyons as classifying spaces","sentence":"We now follow Sen's construction and consider a domain wall configuration of the tachyon such that it condenses to produce a $D8$-brane [ref] .","intent_p":0.9,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":3,"sentences":3,"quotes":[{"arxiv_id":"1004.3972","title":"On The Structure Of The Chan-Paton Factors For D-Branes In Type II Orientifolds","url":"/paper/1004.3972","section":"Non-BPS D-Branes In Type II Superstrings","sentence":"If we set $V'=$ and turn off boundary interaction, our construction has the same Chan-Paton structure and the open string interaction rule as the ones given by Sen, which were first proposed in [ref] and later rationalized in [ref] using the $(-1)^F_L$ orbifold.","intent_p":1.0,"contests_p":null},{"arxiv_id":"1903.00487","title":"Gepner-like boundary states on $T^4$","url":"/paper/1903.00487","section":"Stable non-BPS boundary states","sentence":"They should not be confused with the standard stable non-BPS D$p$-branes of [ref] which are constructed on type II orbifolds and orientifolds and carry conserved (twisted) RR charges.","intent_p":0.99,"contests_p":null},{"arxiv_id":"2512.04977","title":"Thermodynamics vs Teleodynamics: A Cosmological Divide?","url":"/paper/2512.04977","section":"Introduction","sentence":"Also, it should be noted that the “microstate counting\" that appears in the teleodynamic derivation of cosmological horizon entropy [ref] is fundamentally different from the quantum microstate counting underlying black hole entropy in string theory [ref] .","intent_p":0.85,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":2,"sentences":2,"quotes":[{"arxiv_id":"2305.01012","title":"Anomalies and Nonsupersymmetric D-Branes","url":"/paper/2305.01012","section":"D8-Branes and D0-Branes","sentence":"Sen.] the D8-D9 system is tachyonic, so the D8-brane is not entirely stable.) This is an important result of [ref] : Type I superstring theory has D0-branes that are stable, though nonsupersymmetric, because the tachyon is removed by the orientifold projection.","intent_p":0.96,"contests_p":null},{"arxiv_id":"1603.06576","title":"A new 6d fixed point from holography","url":"/paper/1603.06576","section":"Introduction","sentence":"This would be in line with [ref] , where non-BPS $(p-1)$ branes were proven to effectively describe a D$p$–$Dp$ system upon tachyon condesation, this would be consistent with our proposal in section [ref].","intent_p":0.97,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":22,"sentences":22,"quotes":[{"arxiv_id":"2412.17894","title":"Anomaly Inflow and Gauge Group Topology in the 10d Sugimoto String Theory","url":"/paper/2412.17894","section":"Implications for the gauge group toplogy","sentence":"As reviewed more recently [ref] , it is known that stable non-BPS D0-branes in type I, which can be viewed as tachyon condensates from 1-brane/anti-1-brane pairs, carry the spinor representation of $Spin(32)$ [ref] .","intent_p":0.84,"contests_p":null},{"arxiv_id":"2404.15985","title":"Frozen stars: Black hole mimickers sourced by a string fluid","url":"/paper/2404.15985","section":"Born-Infeld effective Lagrangian and BIons","sentence":"The starting point for the analysis in [ref] is Sen's effective action for the decay of unstable $D$-branes; specifically, at the end of tachyon condensation and near the minimum of the tachyon potential, where it is vanishing [ref] .","intent_p":0.84,"contests_p":null},{"arxiv_id":"1906.06078","title":"A Note on the dS Swampland Conjecture, Non-BPS branes and K-theory","url":"/paper/1906.06078","section":"Non-BPS branes","sentence":"It is known that due to the orientifold projection there can exist stable non-BPS branes (see for instance the review [ref] ) that correspond to torsional K-theory groups [ref] .","intent_p":0.81,"contests_p":null},{"arxiv_id":"2606.08767","title":"Fire at the Tip of the Throat: Hagedorn Phase after brane-antibrane inflation?","url":"/paper/2606.08767","section":"Introduction","sentence":"Brane-antibrane inflation [ref] is a particularly sharp example: unlike ordinary single-field models, where reheating is usually modeled by perturbative inflaton decay, D3/$D3$ inflation ends when the open string stretched between the brane and antibrane becomes tachyonic [ref] and the pair annihilates.","intent_p":0.98,"contests_p":null},{"arxiv_id":"2312.11634","title":"String Theory in Rolling Tachyon Vacuum","url":"/paper/2312.11634","section":"D-instantons","sentence":"The unstable D-brane system under consideration is either a non-BPS D-brane [ref] or a coincident D-brane - anti-D-brane system.","intent_p":0.86,"contests_p":null}]}],"unlabelled_sentences":77},"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":{"arxiv_id":"hep-th/9904207","kind":"model","paper_version":1,"prompt_version":"held-up-v3.5","generated_at":"2026-10-27T20:05:28+00:00","loaded_at":"2026-10-28T01:03:41.376106+00:00","evidence":"substantial","account":[],"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":1,"entries":[{"p":0.9,"quote":null,"citing":[{"self":false,"year":2019,"title":"Topological Superconductors on Superstring Worldsheets","arxiv_id":"1911.11780"}],"verified":true,"paraphrase":"Followed this paper's construction to consider a domain wall configuration of the tachyon condensing to produce a D8-brane."}],"papers_all":2,"self_papers":0,"self_entries":[]}],"counts":{"by_kind":{"comparison":3,"method_or_tool":2,"supports_this_paper":3},"dropped":{"relied_on":0,"unknown_ids":0,"account_lines":0,"contest_vetoed":0,"below_threshold":0,"contest_drawback":0,"contest_without_basis":0,"contest_not_one_sentence":0,"contest_on_group_citation":0},"papers_read":11,"self_papers":2,"citing_papers":70,"sentences_read":14,"citing_sentences":101,"unambiguous_read":14,"typed_independent":8,"independent_papers":68,"by_kind_independent":{"comparison":3,"method_or_tool":2,"supports_this_paper":3}},"input_sha256":"1a69e9949e57e37d2759e24ced8ac2c91f0a28041ec8e6f85eeccb7b45c2c5d7","method":"For a paper with five or more citing arXiv papers, Pith selected up to 40 citing sentences its citation classifier typed, read those whose citation markers point at this paper alone, and wrote one paraphrase for each later paper in each group, each resting on one sentence. 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A paper with fewer citing papers gets a line counted by code, which names uses only: a later paper whose only label is a contest is counted as not described.","line":null,"summary":"1 later paper by other authors is listed below: 1 used its method or tool."},"_links":{"html":"https://pith.science/paper/hep-th/9904207"}}