cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.25625/kxuo3g/qzsxar
title: results_msd.pkl
DOI: 10.25625/kxuo3g/t6ujjf
title: results_tau0p0006.pkl
DOI: 10.25625/kxuo3g/xnt2ae
title: results_passive.txt
DOI: 10.25625/kxuo3g/0fas7a
title: final_result.txt
DOI: 10.25625/kxuo3g/cg5ddo
title: results_1s_reversed.pkl
DOI: 10.25625/kxuo3g/vzzkct
title: results_tau0p002.pkl
DOI: 10.25625/kxuo3g/wcq40a
title: results_tau0p0006_reversed.pkl
DOI: 10.25625/kxuo3g/haafxq
title: results_tau0p0001.pkl
DOI: 10.25625/kxuo3g/o991pq
title: active_new.pkl
DOI: 10.25625/kxuo3g/pa4mms
title: amplitude_002.mat
DOI: 10.25625/kxuo3g/vvcgag
title: amplitude_001.mat
DOI: 10.25625/kxuo3g/1kxnwu
title: amplitude_007.mat
DOI: 10.25625/kxuo3g/dp40d5
title: active.txt
DOI: 10.25625/kxuo3g/ipynk3
title: amplitude_004.mat
DOI: 10.25625/kxuo3g/nm74su
title: amplitude_008.mat
DOI: 10.25625/kxuo3g/wx0igk
title: amplitude_005.mat
DOI: 10.25625/kxuo3g/1ttv2s
title: amplitude_010.mat
DOI: 10.25625/kxuo3g/lebwzp
title: amplitude_006.mat
DOI: 10.25625/kxuo3g/m764qw
title: amplitude_009.mat
DOI: 10.25625/kxuo3g/v1e4ip
title: amplitude_000.mat
DOI: 10.25625/kxuo3g/vcz7e9
title: amplitude_003.mat
DOI: 10.25625/kxuo3g/cp8hcx
title: results_1s.pkl
DOI: 10.25625/kxuo3g/moevtv
title: Force_Dissi.pkl
DOI: 10.25625/kxuo3g/o5cr7a
title: results_tau0p01.pkl
DOI: 10.25625/kxuo3g/zecpfc
title: combined_new.pkl
DOI: 10.25625/kxuo3g/4e65jw
title: results_passive.txt
DOI: 10.25625/kxuo3g/e1qyrj
title: amplitude_000_mbr.pkl
DOI: 10.25625/kxuo3g/npdgm2
title: amplitude_001.mat
DOI: 10.25625/kxuo3g/psdodj
title: amplitude_001_mbr.pkl
DOI: 10.25625/kxuo3g/ujmmlg
title: passive_new.pkl
DOI: 10.57702/q11z1d17
title: LDM ORKG Feature

description: By adding the DOI of the paper that defines the dataset to the LDM, a link to the corresponding paper in the ORKG will added to the dataset
DOI: 10.25625/kxuo3g/d20r6c
title: amplitude_000.mat
DOI: 10.25625/kxuo3g/jy90ry
title: results_tau0p0006.pkl
DOI: 10.25625/kxuo3g/nimefc
title: results_tau0p002.pkl
DOI: 10.25625/kxuo3g/vefh6b
title: results_msd.pkl
DOI: 10.25625/kxuo3g/4r9uua
title: results_tau0p0001.pkl
DOI: 10.25625/kxuo3g/kgijzl
title: final_result.txt
DOI: 10.25625/kxuo3g/oc9yae
title: results_tau0p0006_reversed.pkl
DOI: 10.25625/kxuo3g/ws6woc
title: results_1s_reversed.pkl
DOI: 10.25625/kxuo3g/zgd4ge
title: active_new.pkl
DOI: 10.25625/kxuo3g/kdoil7
title: amplitude_002.mat
DOI: 10.25625/kxuo3g/kmemni
title: amplitude_007.mat
DOI: 10.25625/kxuo3g/mmebcm
title: amplitude_008.mat
DOI: 10.25625/kxuo3g/uitcpm
title: amplitude_001.mat
DOI: 10.25625/kxuo3g/574wec
title: amplitude_004.mat
DOI: 10.25625/kxuo3g/isbyzi
title: active.txt
DOI: 10.25625/kxuo3g/qjhmnx
title: amplitude_005.mat
DOI: 10.25625/kxuo3g/qvd7d9
title: amplitude_009.mat
DOI: 10.25625/kxuo3g/rc9cnr
title: amplitude_010.mat
DOI: 10.25625/kxuo3g/ap8rfv
title: Force_Dissi.pkl
DOI: 10.25625/kxuo3g/jt1anm
title: amplitude_006.mat
DOI: 10.25625/kxuo3g/k5goo7
title: results_tau0p01.pkl
DOI: 10.25625/kxuo3g/ooq4i6
title: amplitude_000.mat
DOI: 10.25625/kxuo3g/ptsggp
title: amplitude_003.mat
DOI: 10.25625/kxuo3g/0hr7zo
title: amplitude_001_mbr.pkl
DOI: 10.25625/kxuo3g/mjxxco
title: results_1s.pkl
DOI: 10.25625/kxuo3g/qcdfbw
title: passive_new.pkl
DOI: 10.25625/kxuo3g/vapply
title: combined_new.pkl
DOI: 10.25625/kxuo3g/nkdnaa
title: results_passive.txt
DOI: 10.25625/kxuo3g/owzhfp
title: amplitude_001.mat
DOI: 10.25625/kxuo3g/rph21y
title: amplitude_002.mat
DOI: 10.25625/kxuo3g/rvajko
title: amplitude_000_mbr.pkl
DOI: 10.25625/kxuo3g/vrmub8
title: results_1s.pkl
DOI: 10.25625/kxuo3g/6nhvnt
title: amplitude_000.mat
DOI: 10.25625/kxuo3g/hiey8v
title: results_msd.pkl
DOI: 10.25625/kxuo3g/sn6jyz
title: results_tau0p0006.pkl
DOI: 10.25625/kxuo3g/wjl2t1
title: amplitude_002_mbr.pkl
DOI: 10.25625/kxuo3g/jgxa7p
title: van_hove.npy
DOI: 10.25625/kxuo3g/tmu1n4
title: final_result.npy
DOI: 10.25625/kxuo3g/1l9jub
title: results_tau0p002.pkl
DOI: 10.25625/kxuo3g/b9ju7c
title: results_1s_reversed.pkl
DOI: 10.25625/kxuo3g/f0rdmv
title: results_tau0p0006_reversed.pkl
DOI: 10.25625/kxuo3g/mrejzx
title: final_result.txt
DOI: 10.25625/kxuo3g/bfhlmw
title: results_tau0p0001.pkl
DOI: 10.25625/kxuo3g/ezclbf
title: active_new.pkl
DOI: 10.25625/kxuo3g/okctvd
title: amplitude_002.mat
DOI: 10.25625/kxuo3g/zaeplf
title: amplitude_001.mat
DOI: 10.25625/kxuo3g/ci9dzx
title: amplitude_008.mat
DOI: 10.25625/kxuo3g/gzkhur
title: amplitude_004.mat
DOI: 10.25625/kxuo3g/n2fpqn
title: amplitude_007.mat
DOI: 10.25625/kxuo3g/zk5uhg
title: amplitude_005.mat
DOI: 10.25625/kxuo3g/6n9ax5
title: active.txt
DOI: 10.25625/kxuo3g/p04xfz
title: amplitude_010.mat
DOI: 10.25625/kxuo3g/779eax
title: amplitude_006.mat
DOI: 10.25625/kxuo3g/c1tzsy
title: amplitude_009.mat
DOI: 10.25625/kxuo3g/mp5ydz
title: amplitude_000.mat
DOI: 10.25625/kxuo3g/n5ncug
title: amplitude_003.mat
DOI: 10.25625/kxuo3g/8vg491
title: slope_y.mat
DOI: 10.25625/kxuo3g/azrndy
title: slope_z.mat
DOI: 10.25625/kxuo3g/ciiaio
title: results_tau0p01.pkl
DOI: 10.25625/kxuo3g/cylf4g
title: z_slope.fig
DOI: 10.25625/kxuo3g/iwa2lq
title: slope_x.mat
DOI: 10.25625/kxuo3g/88n31f
title: Force_Dissi.pkl
DOI: 10.25625/kxuo3g/9py79q
title: combined_new.pkl
DOI: 10.25625/kxuo3g/ndyd7m
title: results_1s.pkl
DOI: 10.25625/kxuo3g/yfskat
title: passive_new.pkl
DOI: 10.25625/kxuo3g/3xgtpx
title: amplitude_002.mat
DOI: 10.25625/kxuo3g/an6f6c
title: amplitude_000_mbr.pkl
DOI: 10.25625/kxuo3g/wgdygv
title: amplitude_001_mbr.pkl
DOI: 10.25625/kxuo3g/zn4toc
title: amplitude_001.mat
DOI: 10.25625/kxuo3g/9oe9fq
title: results_passive.txt
DOI: 10.25625/kxuo3g/exfvtf
title: amplitude_000.mat
DOI: 10.25625/kxuo3g/sd0wg7
title: amplitude_002_mbr.pkl
DOI: 10.25625/kxuo3g/wxpg7l
title: results_1s.pkl
DOI: 10.25625/kxuo3g/6esshm
title: results_tau0p0006_reversed.pkl
DOI: 10.25625/kxuo3g/f86ffv
title: results_tau0p0006.pkl
DOI: 10.25625/kxuo3g/jodbqs
title: results_msd.pkl
DOI: 10.25625/kxuo3g/ssnelz
title: results_1s_reversed.pkl
DOI: 10.25625/kxuo3g/ugur3i
title: results_tau0p002.pkl
DOI: 10.25625/kxuo3g/4etzsq
title: active_new.pkl
DOI: 10.25625/kxuo3g/hokvdu
title: results_tau0p0001.pkl
DOI: 10.25625/kxuo3g/kldslj
title: amplitude_002.mat
DOI: 10.25625/kxuo3g/v5iz8o
title: final_result.txt
DOI: 10.25625/kxuo3g/fkhtr3
title: amplitude_007.mat
DOI: 10.25625/kxuo3g/gjvjjy
title: amplitude_008.mat
DOI: 10.25625/kxuo3g/ooxpwi
title: amplitude_001.mat
DOI: 10.25625/kxuo3g/cbcv5v
title: amplitude_009.mat
DOI: 10.25625/kxuo3g/lo6ik3
title: amplitude_010.mat
DOI: 10.25625/kxuo3g/pvshgw
title: amplitude_004.mat
DOI: 10.25625/kxuo3g/wzabgm
title: active.txt
DOI: 10.25625/kxuo3g/ymp8uf
title: amplitude_005.mat
DOI: 10.25625/kxuo3g/0kgrgq
title: amplitude_003.mat
DOI: 10.25625/kxuo3g/bix93d
title: amplitude_000.mat
DOI: 10.25625/kxuo3g/hm1ki8
title: amplitude_006.mat
DOI: 10.25625/kxuo3g/psuzbl
title: results_tau0p01.pkl
DOI: 10.25625/kxuo3g/dqhpr1
title: combined_new.pkl
DOI: 10.25625/kxuo3g/ekzylh
title: results_1s.pkl
DOI: 10.25625/kxuo3g/s7bm8f
title: passive_new.pkl
DOI: 10.25625/kxuo3g/vspcui
title: Force_Dissi.pkl
DOI: 10.25625/kxuo3g/e2dgkh
title: amplitude_001_mbr.pkl
DOI: 10.25625/kxuo3g/fk6ggz
title: amplitude_000_mbr.pkl
DOI: 10.25625/kxuo3g/qhcznv
title: amplitude_002.mat
DOI: 10.25625/kxuo3g/qmb2su
title: amplitude_001.mat
DOI: 10.25625/kxuo3g/47d7wh
title: amplitude_002_mbr.pkl
DOI: 10.25625/kxuo3g/bgycqx
title: mcd.pufo
DOI: 10.25625/kxuo3g/melqbg
title: results_passive.txt
DOI: 10.25625/kxuo3g/nypzpu
title: amplitude_000.mat
DOI: 10.25625/kxuo3g/f0tnki
title: results_tau0p0006_reversed.pkl
DOI: 10.25625/kxuo3g/jmd39o
title: results_tau0p002.pkl
DOI: 10.25625/kxuo3g/s3wkkr
title: results_tau0p0006.pkl
DOI: 10.25625/kxuo3g/wczkdq
title: results_msd.pkl
DOI: 10.25625/kxuo3g/44fbmi
title: final_result.txt
DOI: 10.25625/kxuo3g/fdlioh
title: results_1s_reversed.pkl
DOI: 10.25625/kxuo3g/kxu26a
title: amplitude_002.mat
DOI: 10.25625/kxuo3g/qwwe5x
title: active_new.pkl
DOI: 10.25625/kxuo3g/vqeinr
title: results_tau0p0001.pkl
DOI: 10.25625/kxuo3g/klugyv
title: amplitude_008.mat
DOI: 10.25625/kxuo3g/sjzub6
title: amplitude_007.mat
DOI: 10.25625/kxuo3g/v6kdkm
title: amplitude_001.mat
DOI: 10.25625/kxuo3g/z6qdv7
title: amplitude_004.mat
DOI: 10.25625/kxuo3g/b3u32r
title: amplitude_005.mat
DOI: 10.25625/kxuo3g/eb1sv6
title: active.txt
DOI: 10.25625/kxuo3g/jqx8jb
title: amplitude_009.mat
DOI: 10.25625/kxuo3g/vhy4e8
title: amplitude_010.mat
DOI: 10.25625/kxuo3g/9t41ys
title: amplitude_000.mat
DOI: 10.25625/kxuo3g/qkgblh
title: amplitude_006.mat
DOI: 10.25625/kxuo3g/gnaz4m
title: amplitude_003.mat
DOI: 10.25625/kxuo3g/kibawg
title: combined_new.pkl
DOI: 10.25625/kxuo3g/koubz9
title: Force_Dissi.pkl
DOI: 10.25625/kxuo3g/z3zjdp
title: results_1s.pkl
DOI: 10.25625/kxuo3g/ziunwp
title: results_tau0p01.pkl
DOI: 10.25625/kxuo3g/du6zug
title: amplitude_001_mbr.pkl
DOI: 10.25625/kxuo3g/kjgcmf
title: passive_new.pkl
DOI: 10.25625/kxuo3g/mrftbx
title: amplitude_001.mat
DOI: 10.25625/kxuo3g/sjhp0g
title: amplitude_000_mbr.pkl
DOI: 10.25625/kxuo3g/ste2zl
title: amplitude_002.mat
DOI: 10.25625/kxuo3g/h4dvh3
title: results_passive.txt
DOI: 10.25625/kxuo3g/isilav
title: mcd.pufo
DOI: 10.25625/kxuo3g/luhkyh
title: amplitude_000.mat
DOI: 10.25625/kxuo3g/ovaoci
title: amplitude_002_mbr.pkl
DOI: 10.25625/kxuo3g/2oqvfa
title: results_1s_reversed.pkl
DOI: 10.25625/kxuo3g/3i32t0
title: results_msd.pkl
DOI: 10.25625/kxuo3g/dgprjx
title: results_tau0p0006.pkl
DOI: 10.25625/kxuo3g/mowc2t
title: results_tau0p002.pkl
DOI: 10.25625/kxuo3g/xxqn8k
title: results_tau0p0006_reversed.pkl
DOI: 10.25625/kxuo3g/2b3trv
title: active_new.pkl
DOI: 10.25625/kxuo3g/7fqush
title: final_result.txt
DOI: 10.25625/kxuo3g/e1m1vl
title: amplitude_002.mat
DOI: 10.25625/kxuo3g/qgs0sg
title: results_tau0p0001.pkl
DOI: 10.25625/kxuo3g/tshovd
title: amplitude_001.mat
DOI: 10.25625/kxuo3g/3oisik
title: amplitude_008.mat
DOI: 10.25625/kxuo3g/9ho1et
title: amplitude_007.mat
DOI: 10.25625/kxuo3g/k4etgl
title: amplitude_004.mat
DOI: 10.25625/kxuo3g/tfhaye
title: amplitude_005.mat
DOI: 10.25625/kxuo3g/dxjngg
title: amplitude_009.mat
DOI: 10.25625/kxuo3g/e8j7h8
title: amplitude_010.mat
DOI: 10.25625/kxuo3g/hkgmfo
title: amplitude_006.mat
DOI: 10.25625/kxuo3g/o8sr5a
title: active.txt
DOI: 10.25625/kxuo3g/yrvqk7
title: amplitude_000.mat
DOI: 10.25625/kxuo3g/bdyqxa
title: combined_new.pkl
DOI: 10.25625/kxuo3g/cmphys
title: results_tau0p01.pkl
DOI: 10.25625/kxuo3g/earw5r
title: amplitude_003.mat
DOI: 10.25625/kxuo3g/npluyd
title: results_1s.pkl
DOI: 10.25625/kxuo3g/w27slr
title: Force_Dissi.pkl
DOI: 10.25625/kxuo3g/iuzfpm
title: amplitude_001_mbr.pkl
DOI: 10.25625/kxuo3g/ljymvo
title: passive_new.pkl
DOI: 10.25625/kxuo3g/lkwae3
title: amplitude_000_mbr.pkl
DOI: 10.25625/kxuo3g/ll4fqj
title: amplitude_002.mat
DOI: 10.25625/kxuo3g/teq24s
title: amplitude_001.mat
DOI: 10.25625/kxuo3g/dorqzr
title: amplitude_000.mat
DOI: 10.25625/kxuo3g/n0iwrk
title: mcd.pufo
DOI: 10.25625/kxuo3g/x1b7sd
title: results_passive.txt
DOI: 10.25625/kxuo3g/00o5mn
title: results_tau0p0006.pkl
DOI: 10.25625/kxuo3g/6rrdhd
title: amplitude_002_mbr.pkl
DOI: 10.25625/kxuo3g/fhxbik
title: results_tau0p002.pkl
DOI: 10.25625/kxuo3g/id7le6
title: results_msd.pkl
DOI: 10.25625/kxuo3g/vujszf
title: results_tau0p0006_reversed.pkl
DOI: 10.25625/kxuo3g/0ioi9k
title: final_result.txt
DOI: 10.25625/kxuo3g/3ool90
title: results_1s_reversed.pkl
DOI: 10.25625/kxuo3g/qrd9lp
title: active_new.pkl
DOI: 10.25625/kxuo3g/xbzxyr
title: results_tau0p0001.pkl
DOI: 10.25625/kxuo3g/2vnkfv
title: amplitude_008.mat
DOI: 10.25625/kxuo3g/bnzndh
title: amplitude_001.mat
DOI: 10.25625/kxuo3g/bzvffy
title: amplitude_002.mat
DOI: 10.25625/kxuo3g/id3irb
title: amplitude_007.mat
DOI: 10.25625/kxuo3g/4bvv8p
title: amplitude_009.mat
DOI: 10.25625/kxuo3g/5f7lkp
title: amplitude_005.mat
DOI: 10.25625/kxuo3g/cycyoc
title: active.txt
DOI: 10.25625/kxuo3g/napfya
title: amplitude_010.mat
DOI: 10.25625/kxuo3g/psu2rh
title: amplitude_004.mat
DOI: 10.25625/kxuo3g/dnrgwp
title: amplitude_003.mat
DOI: 10.25625/kxuo3g/dtnrwf
title: amplitude_000.mat
DOI: 10.25625/kxuo3g/gphtty
title: Force_Dissi.pkl
DOI: 10.25625/kxuo3g/hg8iam
title: amplitude_006.mat
DOI: 10.25625/kxuo3g/ma5w9m
title: results_tau0p01.pkl
DOI: 10.25625/kxuo3g/ghk5ip
title: amplitude_001_mbr.pkl
DOI: 10.25625/kxuo3g/ix4uzq
title: results_1s.pkl
DOI: 10.25625/kxuo3g/lnbcre
title: combined_new.pkl
DOI: 10.25625/kxuo3g/udodmk
title: passive_new.pkl
DOI: 10.25625/kxuo3g/0rciyn
title: amplitude_000_mbr.pkl
DOI: 10.25625/kxuo3g/ictfmt
title: amplitude_002.mat
DOI: 10.25625/kxuo3g/v8jqi0
title: results_passive.txt
DOI: 10.25625/kxuo3g/vxxxlw
title: amplitude_001.mat
DOI: 10.25625/kxuo3g/g1xry1
title: results_tau0p0006.pkl
DOI: 10.25625/kxuo3g/qk8kiy
title: amplitude_000.mat
DOI: 10.25625/kxuo3g/ti6jaa
title: amplitude_002_mbr.pkl
DOI: 10.25625/kxuo3g/woaf6w
title: results_msd.pkl
DOI: 10.25625/kxuo3g/yugior
title: mcd.pufo
DOI: 10.25625/kxuo3g/bg5otm
title: results_tau0p0006_reversed.pkl
DOI: 10.25625/kxuo3g/dchhm7
title: results_tau0p002.pkl
DOI: 10.25625/kxuo3g/jaarcl
title: results_1s_reversed.pkl
DOI: 10.25625/kxuo3g/mhjmzk
title: results_tau0p0001.pkl
DOI: 10.25625/kxuo3g/ygsfje
title: final_result.txt
DOI: 10.25625/kxuo3g/3vz8pq
title: active_new.pkl
DOI: 10.25625/kxuo3g/5dv5tz
title: amplitude_001.mat
DOI: 10.25625/kxuo3g/ug2cay
title: amplitude_002.mat
DOI: 10.25625/kxuo3g/4ys0x1
title: amplitude_005.mat
DOI: 10.25625/kxuo3g/czfrfb
title: active.txt
DOI: 10.25625/kxuo3g/ghcqsm
title: amplitude_008.mat
DOI: 10.25625/kxuo3g/itujhb
title: amplitude_007.mat
DOI: 10.25625/kxuo3g/jwpnwu
title: amplitude_004.mat
DOI: 10.25625/kxuo3g/coyfkv
title: amplitude_000.mat
DOI: 10.25625/kxuo3g/nktkje
title: amplitude_006.mat
DOI: 10.25625/kxuo3g/ufyola
title: amplitude_010.mat
DOI: 10.25625/kxuo3g/xutoxe
title: amplitude_009.mat
DOI: 10.25625/kxuo3g/ggdyf6
title: combined_new.pkl
DOI: 10.25625/kxuo3g/jrbscv
title: results_tau0p01.pkl
DOI: 10.25625/kxuo3g/pxxsqv
title: Force_Dissi.pkl
DOI: 10.25625/kxuo3g/rg1eul
title: results_1s.pkl
DOI: 10.25625/kxuo3g/rp6nkb
title: amplitude_003.mat
DOI: 10.25625/kxuo3g/8vhr37
title: amplitude_001.mat
DOI: 10.25625/kxuo3g/aygyf3
title: amplitude_001_mbr.pkl
DOI: 10.25625/kxuo3g/eoa3ja
title: amplitude_002.mat
DOI: 10.25625/kxuo3g/rlsdh3
title: passive_new.pkl
DOI: 10.25625/kxuo3g/5rpq9y
title: amplitude_000_mbr.pkl
DOI: 10.25625/kxuo3g/p1d16i
title: results_passive.txt
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DOI: 10.25625/kxuo3g/ipianl
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DOI: 10.25625/kxuo3g/ocfycg
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DOI: 10.25625/kxuo3g/aommnq
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DOI: 10.25625/kxuo3g/v6o24h
title: amplitude_001.mat
DOI: 10.25625/kxuo3g/4m26lz
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DOI: 10.25625/kxuo3g/gtbyz0
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DOI: 10.25625/kxuo3g/u4bawi
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DOI: 10.25625/kxuo3g/x0ecft
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DOI: 10.25625/kxuo3g/2f9zpj
title: combined_new.pkl
DOI: 10.25625/kxuo3g/cjfank
title: amplitude_001_mbr.pkl
DOI: 10.25625/kxuo3g/mvkqgc
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DOI: 10.25625/kxuo3g/obgrlb
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DOI: 10.25625/kxuo3g/nhunzc
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DOI: 10.25625/kxuo3g/whetuc
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DOI: 10.25625/kxuo3g/xa5iax
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DOI: 10.25625/kxuo3g/7bvfx7
title: amplitude_002_mbr.pkl
DOI: 10.25625/kxuo3g/hg76fu
title: results_msd.pkl
DOI: 10.25625/kxuo3g/oqkyma
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DOI: 10.25625/kxuo3g/pmscxd
title: amplitude_000.mat
DOI: 10.25625/kxuo3g/zyquup
title: results_tau0p0006.pkl
DOI: 10.25625/kxuo3g/3mf0nz
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DOI: 10.25625/kxuo3g/dkldb6
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DOI: 10.25625/kxuo3g/mesrjj
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DOI: 10.25625/kxuo3g/cpulcm
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DOI: 10.25625/kxuo3g/i1cgux
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DOI: 10.25625/kxuo3g/mahwa5
title: amplitude_001.mat
DOI: 10.25625/kxuo3g/zhfau7
title: results_passive.txt
DOI: 10.25625/kxuo3g/ghnyaj
title: results_msd.pkl
DOI: 10.25625/kxuo3g/j4n1l9
title: mcd.pufo
DOI: 10.25625/kxuo3g/oexp1r
title: amplitude_000.mat
DOI: 10.25625/kxuo3g/yliuhy
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DOI: 10.25625/kxuo3g/ci1tgx
title: results_tau0p0006.pkl
DOI: 10.25625/kxuo3g/dfowb3
title: results_1s_reversed.pkl
DOI: 10.25625/kxuo3g/mmnhog
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DOI: 10.25625/kxuo3g/rv2hgl
title: results_tau0p002.pkl
DOI: 10.25625/kxuo3g/bsycht
title: results_tau0p0001.pkl
DOI: 10.25625/kxuo3g/cl4lai
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DOI: 10.25625/kxuo3g/pqjjs5
title: amplitude_001.mat
DOI: 10.25625/kxuo3g/tp53hz
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DOI: 10.25625/kxuo3g/vvdev8
title: final_result.txt
DOI: 10.5281/zenodo.11369779
title: Supplementary dataset for "Magnetic recording fidelity of basalts through 3D nanotomography, 2024"

description: This repository contains raw data and scripts needed to reproduce the results presented in "Magnetic recording fidelity of basalts through 3D nanotomography, 2024". These include slice-and-view image stacks (VesuviusSnVTiffStack.tif for the Vesuvius dataset and HeklaSnVTiffStack.tif for the Hekla Volume) for the samples discussed in the manuscript. These were used to generate 3D meshes of magnetite grains in the volume using the methodology described in the manuscript. Individual Meshes Vesuvius.7z and Individual Meshes Hekla.7z contain the individual 3D mesh .pat files, while Hekla Full Volume.stl and Vesuvius Full Volume.stl show full 3D representations of the studied volumes. The individual mesh files can be used as geometry inputs for micromagnetic simulations using the MERRILL suite . Example MERRILL scripts are also included, with LEM_StateMerrilScript.merrill showing an example of a script used to determine the local energy minimum (LEM) state of a magnetic grain and NEB_Merril_Script.merrill showing a script to determine the energy barriers between LEM states used in the calculation of relaxation times. Finally ".csv" files containing grain metrics are also included for both of the studied samples ( HeklaGrainMetrics.csv and VesuviusGrainMetrics.csv ). These contain information on the size of the individual particles, their morphology, the LEM states they support and the energy barries from the NEB calculation.