Paper Citation Record · LEDGER

Magnetization Current Simulation of High Temperature Bulk Superconductors Using A-V-A Formulation and Iterative Algorithm Method: Critical State Model and Flux Creep Model

As of 16 August 2026, this Paper Citation Record lists 6 of 6 outbound references and 0 inbound Pith citation observations for arXiv:1908.04640.

A citation records a reference. It does not transfer a finding from one paper to another.

pith.paper-citation-record.v1
1908.04640 v2

Coverage vector

measured 6 of 6 reference resolution

Typed states for the displayed outbound observations.

Source: paper_references, paper_reference_links, observed 2026-08-14T13:42:30.001189Z

measured 6 of 6 standing notices

One-hop event checks from named stored sources.

Source: scholarly_work_events, retraction_status_cache, observed 2026-08-16T06:30:59.297886+00:00

measured 0 of 0 inbound itemization

Pith citing papers itemized under the disclosed page cap.

Source: paper_references, paper_reference_links

measured 0 of 1 external citation measurements

A source-named dated measurement, never combined with another source.

Source: cited_works

Reference resolution

6 of 6 outbound references displayed

verified exact0
verified fuzzy6
unresolved0
parse uncertain0
malformed identifier0
metadata mismatch0

External citation measurements

No source-named external measurement is stored.

Outbound references

Observation 65a2007f-ad47-4a27-945f-780af271107a · outbound

This paper cites Recent studies show growing interests of using commercial FEM software, in which E-J power law based equations [Manuscript-19/02/2020- K.

Magnetization Current Simulation of High Temperature Bulk Superconductors Using A-V-A Formulation and Iterative Algorithm Method: Critical State Model and Flux Creep Model Recent studies show growing interests of using commercial FEM software, in which E-J power law based equations [Manuscript-19/02/2020- K

Reference 1

Resolution: verified fuzzy; raw_fallback, observed 2026-08-14T13:42:30.129227Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.

Observation e6b8458f-0dc4-4959-838f-bb232319c224 · outbound

This paper cites BFE” command to force their JT, meanwhile, making their eddy current solver inactive in later steps. d) Set the external field to 2B0/N1 at “t=2T1/N1.

Magnetization Current Simulation of High Temperature Bulk Superconductors Using A-V-A Formulation and Iterative Algorithm Method: Critical State Model and Flux Creep Model BFE” command to force their JT, meanwhile, making their eddy current solver inactive in later steps. d) Set the external field to 2B0/N1 at “t=2T1/N1

Reference 2

Resolution: verified fuzzy; raw_fallback, observed 2026-08-14T13:42:30.110186Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.

Observation c244f305-4f87-4080-bfe6-63786f3a2749 · outbound

This paper cites t=2T1/N1.

Magnetization Current Simulation of High Temperature Bulk Superconductors Using A-V-A Formulation and Iterative Algorithm Method: Critical State Model and Flux Creep Model t=2T1/N1

Reference 3

Resolution: verified fuzzy; raw_fallback, observed 2026-08-14T13:42:30.092505Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.

Observation 2a2ea8f2-acd5-4dec-886c-b21caf8f3816 · outbound

This paper cites repeating.

Magnetization Current Simulation of High Temperature Bulk Superconductors Using A-V-A Formulation and Iterative Algorithm Method: Critical State Model and Flux Creep Model repeating

Reference 4

Resolution: verified fuzzy; raw_fallback, observed 2026-08-14T13:42:30.076096Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.

Observation 5a000d33-8dbd-4d89-a225-fabca048dd35 · outbound

This paper cites t=T1”. 5.1. The critical state model 5.1.1. Number of specified load steps – N1 Figure 16 compares the trapped JT in ReBCO bulk at “t=T1.

Magnetization Current Simulation of High Temperature Bulk Superconductors Using A-V-A Formulation and Iterative Algorithm Method: Critical State Model and Flux Creep Model t=T1”. 5.1. The critical state model 5.1.1. Number of specified load steps – N1 Figure 16 compares the trapped JT in ReBCO bulk at “t=T1

Reference 5

Resolution: verified fuzzy; raw_fallback, observed 2026-08-14T13:42:30.059487Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.

Observation d61e67dc-fb9e-475b-80ed-73565c6f80be · outbound

This paper cites This new method is proved feasible to simulate the ReBCO bulk ’s magnetization current during ZFC or FC magnetization for both critical state model and flux creep model.

Magnetization Current Simulation of High Temperature Bulk Superconductors Using A-V-A Formulation and Iterative Algorithm Method: Critical State Model and Flux Creep Model This new method is proved feasible to simulate the ReBCO bulk ’s magnetization current during ZFC or FC magnetization for both critical state model and flux creep model

Reference 6

Resolution: verified fuzzy; raw_fallback, observed 2026-08-14T13:42:30.043058Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.

Pith citing papers

No inbound Pith citation observations are available.