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NMDB and space weather forecasting

Abstract

From the creation of NMDB in 2007 and through the growth in the number of stations and the data accumulation, the ShICRA SB RAS group continuously have used its facilities. For the last years we have created a method for short-term forecasting of intense geomagnetic storms with an advance time 1-2 days. The probability of forecasting is around 80%. We have reported about the method in the previous NMDB: virtual symposium on cosmic ray studies with neutron detectors in 2020. The method is based on the global survey method that was developed in Yakutsk in 1960s and uses the world network of neutron monitors as a single multidirectional device. The method is intended to estimate hourly dynamics of cosmic ray anisotropy in free-space. Note that only with the NMDB creation we managed to implement it in real time mode. Now we started work on creating another method for space weather forecasting by measurements of cosmic ray fluctuations. For this purpose, we use 1-min data of NMDB. In the current report we present the first results of our investigation on forecasting of intense geomagnetic storms with Dst < -50 nT. The results obtained indicate the possibility of developing and implementing in real time a method for predicting strong geophysical manifestations of space weather on the basis of ground-based cosmic ray measurements.

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NMDB and space weather forecasting

Author: Gololobov, Petr Yu.,Starodubtsev, Sergey A.,Grigoryev, Vladislav G.,Zverev, Anton S.
Year: 2023
DOI: 10.38072/2748-3150/p33
Source: https://macau.uni-kiel.de/servlets/MCRFileNodeServlet/macau_derivate_00005425/kiel-up_2748-3150_p33.pdf
Cosmic ay s udies wi h neu on de ec o s | Volume 2 (2023) 81
KIEL-UP • DOI: 10.38072/2748-3150/p33
NMDB and space wea he o ecas ing
Pe Yu. Gololobo , Se gey A. S a odub se , Vladisla G. G igo ye , An on S. Z e e
Co espondence
Yu.G. Sha e Ins i u e o Cosmophysical Resea ch and Ae onomy, Sibe ian B anch o he Russian Academy o
Science, Russia,
[email p o ec ed]u
Keywo ds
cosmic ays; neu on moni o ; magne ohyd odynamic wa es; luc ua ions; u bulence spec um
Abs ac
F om he c ea ion o NMDB in 2007 and h ough he g ow h in he numbe o s a ions and he da a accumula ion,
he ShICRA SB RAS g oup con inuously ha e used i s acili ies. Fo he las yea s we ha e c ea ed a me hod
o sho - e m o ecas ing o in ense geomagne ic s o ms wi h an ad ance ime 1-2 days. The p obabili y o
o ecas ing is a ound 80%. We ha e epo ed abou he me hod in he p e ious NMDB: i ual symposium on
cosmic ay s udies wi h neu on de ec o s in 2020. The me hod is based on he global su ey me hod ha was
de eloped in Yaku sk in 1960s and uses he wo ld ne wo k o neu on moni o s as a single mul idi ec ional
de ice. The me hod is in ended o es ima e hou ly dynamics o cosmic ay aniso opy in ee-space. No e
ha only wi h he NMDB c ea ion we managed o implemen i in eal ime mode. Now we s a ed wo k on
c ea ing ano he me hod o space wea he o ecas ing by measu emen s o cosmic ay luc ua ions. Fo his
pu pose, we use 1-min da a o NMDB. In he cu en epo we p esen he i s esul s o ou in es iga ion
on o ecas ing o in ense geomagne ic s o ms wi h Ds < -50 nT. The esul s ob ained indica e he possibili y
o de eloping and implemen ing in eal ime a me hod o p edic ing s ong geophysical mani es a ions o
space wea he on he basis o g ound-based cosmic ay measu emen s.
1. In oduc ion
The sea ch o e ec i e and imely space wea he o ecas ing is one o he mos impo an asks o so-
la - e es ial ela ionships. This is due o he ac ha i s change and subsequen impac on he Ea h
is po en ially nega i e. Fi s o all, his conce ns geomagne ic s o ms, which can lead o a ious kinds
o nega i e e ec s on echnological sys ems as, o example, communica ion dis up ion o powe g id
ailu es. Wi h he de elopmen o mode n elec onic echnology and space explo a ion, he ele ance o
sol ing his issue is as high as e e .
Obse a ions o he s a e o nea -Ea h ou e space a e adi ionally ca ied ou by di ec measu e-
men s o he pa ame e s o he in e plane a y medium wi h a ious de ec o s ins alled on boa d space-
c a . A he same ime, spacec a , as a ule, a e loca ed in ela i e p oximi y o he Ea h and a e able
o p edic wi h g ea accu acy he mani es a ions o changes in space wea he on Ea h o abou 1 hou .
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In his sho ime, i is p ac ically impossible o ake eal p e en i e measu es o any kind. On he o he
hand, his is possible i , o he pu poses o space wea he o ecas ing, g ound-based CR measu emen s
a e used, which, due o hei long mean ee pa hs, ca y in o ma ion abou he p ope ies o he in e pla-
ne a y medium on la ge scales. A simila app oach o space wea he o ecas ing has been de eloped by
many esea che s (as an example, some o hem can be men ioned (Ma omichalaki e al. 2006; Biebe
e al. 2004; Kudela e al. 2000)).
Since he ea ly 2000s we a e wo king on de eloping a space wea he o ecas ing echnique based
on g ound-based measu emen s o cosmic ays (G igo ye e al. 2011; G igo ye e al. 2015). Thus, he
c ea ion o a da abase o neu on moni o s ins alled on he wo ldwide ne wo k o CR s a ions (NMDB)
in 2007, which p o ides eal- ime measu emen da a, allowed us o begin he p ac ical implemen a ion
o he space wea he o ecas ing algo i hm based on he global su ey me hod de eloped in Yaku sk
a he end o he 1960s. In pa icula , some o he esul s o his wo k we e p esen ed a he p e ious
NMDB symposium in 2020 (Gololobo e al. 2020). I was shown ha he spa ial-angula dis ibu ion
o CR expe iences changes ha a e ypical only o pe iods be o e he a i al o geoe ec i e sola wind
dis u bances, which can lead o s ong geomagne ic s o ms wi h Ds < -50 nT. In his case, 1 hou CR
egis a ion da a a e used, and he me hod de eloped by us makes i possible o p edic such s o ms wi h
80% p obabili y.
Ano he app oach o space wea he o ecas ing is o use he eco ding CR in ensi y luc ua ions (G i-
go ye e al. 2008). CR luc ua ions a e unde s ood as non-s a iona y a ia ions wi h pe iods o less han
2-3 hou s (wi h a equency o mo e han 10-4 Hz), which a e obse ed only du ing la ge-scale sola wind
dis u bances. In connec ion wi h his ci cums ance, he p esen wo k is de o ed o he de elopmen o
a me hod o p edic ing space wea he om g ound-based measu emen s o CR in ensi y luc ua ions.
2. CR in ensi y luc ua ions
As es ablished back in he 1970s, CR luc ua ions a ise as a esul o modula ion o high-ene gy CR luxes
(E>1 GeV) by magne ohyd odynamic (MHD) wa es. In his case, he ela ionship be ween he aniso opic
pa o he CR dis ibu ion unc ion and Al én wa es was conside ed by Owens (1974). In his wo k, i
was shown ha he powe spec a o luc ua ions o CRs P
CR
(
ν, μ, V
)
and he in e plane a y magne ic ield
(IMF) ans e se componen s P
B⊥
(
ν
)
a e ela ed by he ela ion:
P
CR
(
ν, μ, V
)
_
j
0
2
= C
(
ν, μ
)
P
B⊥
(
ν
)
_
B
0
2
δ
∥
2  ∼  10
−6
P
B⊥
(
ν
)
_
B
0
2
whe e B
0 is he a e age in ensi y o he IMF, j
0 is he CR lux, V is he CR eloci y in cm·s-1, δ
∥  ∼
U
⁄
c  ∼  10
−3
is he CR lux aniso opy along he magne ic ield, U and c a e he sola wind and ligh eloci ies, C ( ν, μ )
is a pa ame e ha akes in o accoun he nonlinea in e ac ion nea esonan equencies, μ is he pi ch
angle o he pa icle, ν is he equency.
On he o he hand, in he wo k o Be ezhko and S a odub se (Be ezhko & S a odub se 1988) i was
es ablished ha in he p esence o as magne osonic wa es (FMW) in he sola wind, which a e capable
o modula ing he main, iso opic pa o he CR dis ibu ion unc ion, he spec a o CR luc ua ions and
he IMF modulus a e ela ed by he ela ion:
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P
CR
(
ν
)
_
j
0
2
=
[
(
γ + 2
)
C
a
(
C
W
+ Usinφ
)
_________________
3π
√
_
2
k
⊥
ν
]
2
P
B
(
ν
)
_
B
0
2
∼
(
10
−2
÷ 1
)
P
B
(
ν
)
_
B
0
2
whe e he wa e eloci y is C
W  =
√
_
(
C
a
2 + C
S
2
)
, C
a and C
S a e he eloci ies o he Al en and magne osonic
wa es, k
⊥ is he ans e se pa icle di usion coe icien , φ is he angle be ween he sola wind di ec ion
and he IMF o ce lines.
In Be ezhko & S a odub se (1988) i was shown o a numbe o e en s ha i is ela ion (2) ha is
applicable o desc ibe he spec um o CR luc ua ions in he equency ange abo e 10-4 Hz, which is
di ec e idence o he gene a ion o CR luc ua ions p ecisely by FMS wa es. Mo eo e , e idence was
gi en ha his ype o MHD wa es is gene a ed by lows o sup a he mal pa icles, which a e o en
obse ed ahead o he on s o in e plane a y shock wa es. And since hey o en cause s ong geoma-
gne ic s o ms, he e y egis a ion o CR luc ua ions in g ound-based de ec o da a can be an e ec i e
p edic o o hese s o ms
.
3. Me hod
To de e mine CR in ensi y luc ua ions in he ine ial pa o he u bulence spec um, we use 1-minu e
measu emen s. I should be no ed ha he huge a ay o measu emen da a om neu on moni o s wi h
high empo al esolu ion, accumula ed by he wo ld ne wo k o CR s a ions, is p ac ically no used in any
way, excep o he analysis o a e cases o GLE e en s, and lies unclaimed. He e we use ba ome ic-co -
ec ed 1-min da a om he Yaku sk (62.02ºN, 129.72ºE, R
c =1.65 GV) and Tixie Bay (71.60ºN, 128.90ºE,
R
c =0.53 GV) neu on moni o s. These s a ions a e pa o he Russian na ional ne wo k o CR g ound s a-
ions, whose da a a e ansmi ed o he NMDB se e in eal ime. Bo h o hese s a ions a e loca ed ai ly
close o he same me idian, and he asymp o ic angles o a i al o pa icles a hem coincide ai ly well.
Fluc ua ions in CR and he in e plane a y medium we e analyzed using he s anda d Blackman-Tukey
me hod (Blackman & Tukey 1958). In pa icula , o each s a ion we calcula ed au o-spec a o CR powe 
P
xx
(
)
P
xx
(
ν
)
= 2∫ w
(
τ
)
R
xx
(
τ
)
cos
(
2πντ
)
dτ
whe e R xx (τ) is an au oco a iance unc ion, w (τ) is Tukey’s co ela ion window, equal o
w
T
(
τ
)
=
1
_
2
(
1 + cos
πτ
_
m
)
, τ ≤ m
w
T
(
τ
)
= 0,τ > m
Also, c oss powe spec a o CR luc ua ions we e calcula ed o bo h s a ions. I s alues can be w i en as
he sum o he eal and imagina y pa s o he spec um componen s:
P
xy
(
ν
)
=  C
xy
(
ν
)
+ j ⋅ Q
xy
(
ν
)
,
whe e C xy (ν) and Q xy (ν) a e cospec um and quad a u e spec um.
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In his case, along wi h he spec al powe o he signal, he cohe ence coe icien Г
xy was de e mined,
which de e mines he igh ness o he connec ion be ween he luc ua ions o wo quan i ies. The cohe -
ence coe icien is de ined as he posi i e alue o he squa e oo o he cohe ence unc ion:
Γ
xy
(
ν
)
= +
√
_
P
xy
2
_
P
xx P
yy
.
The cohe ence ac o can also be used o de e mine he ype o MHD wa e. Fo example, i is known ha
Al en wa es a e cha ac e ized by high alues o he cohe ence coe icien be ween he s eng h o he
IMF and he sola wind eloci y, FMW — be ween he IMF s eng h and he sola wind densi y, and slow
magne osonic wa es — be ween he sola wind eloci y and densi y.
4. Resul s ob ained
We ha e analyzed mo e han 100 cases o obse a ion in he 23 d and 24 h cycles o sola ac i i y o
s ong geomagne ic s o ms cha ac e ized by Ds <-50 nT. He e, as an example, we will conside only one
e en o a s ong geomagne ic s o m wi h a Ds -index o abou -80 nT ha occu ed on Sep embe 20,
2015. Ou esul s a e shown in Figu e 1. I s analysis shows ha in he ime pe iod 2015 Sep embe 18
(00:01 UT)-19 (00:00UT), a clea inc ease in he cohe ence coe icien Γ
Bn was obse ed in he equency
ange <10-3 Hz o he conside ed spec um, which indica es he p edominan ole o FMS wa es in he
o ma ion o he spec um o IMF luc ua ions.
Fig.1: Powe spec al densi ies PB and PFMS, as well as cohe ence coe icien s be ween ΓBn o di e en ime pe iods.
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O e he same ime pe iods, we de e mined he cohe ence coe icien s be ween luc ua ions in he CR
in ensi y eco ded a he Yaku sk and Tixie Bay Γ
NM s a ions. The esul s ob ained a e p esen ed in Figu e
2. I is ob ious ha Γ
NM also shows high alues in he low equency egion. Thus, high alues o he co-
he ence coe icien be ween neu on moni o s a ions can indica e bo h he p esence o FMS wa es in he
sola wind and an impending geomagne ic s o m.
Le us conside he possibili y o using he cohe ence coe icien Γ
NM as a geomagne ic dis u bance p e-
dic o . To do his, we will conside he highes alues o he cohe ence coe icien Γ
NM in he en i e spec-
um ange wi h a s ep o 1 hou o Sep embe 18-20, 2015. The esul s ob ained a e shown in Figu e 3.
As can be seen om Figu e 3 (le panel), 18 hou s be o e he s o m ha began on Sep embe 20, 2015,
high alues o Γ
NM we e obse ed. A he same ime, he esul s o measu emen s o he luxes o supe -
he mal p o ons ca ied ou on he WIND spacec a (Figu e 3, igh panel, h ps://omniweb.gs c.nasa.
Fig. 2: Cohe ence coe icien be ween CR luc ua ions acco ding o measu emen s o neu on moni o s Yaku sk and
Tixie Bay
Γ
NM
.
Fig. 3. Le panel: cohe ence coe icien s
Γ
NM
and Ds -index o Sep embe 18-20, 2020. Righ panel: measu emen da a
o p o on luxes in 9 di e en ial ene gy channels (P1 = 0.130-0.163 MeV, P2 = 0.163-0.233 MeV, P3 = 0.233-0.325 MeV,
P4 = 0.325–0.457 MeV, P5 = 0.457–0.653 MeV, P6 = 0.653–0.884 MeV, P7 = 0.884–1.270 MeV, P8 = 1.270–1.740 MeV, P9 =
1.740–2.510 MeV) by he WIND spacec a o e a pe iod o 18-20 Sep embe 2015.

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go / o m/sc_me ge_min1.h ml) show ha hei g ow h coincides wi h he obse a ion o high alues o
Γ
NM . Consequen ly, supe he mal p o ons can be a sou ce o FMS wa es.
Thus, aking in o accoun he beha io o 𝚪
NM in o he e en s, i can be assumed ha i is an e ec i e
p edic o o geomagne ic dis u bances o medium- e m space wea he o ecas ing.
5. Conclusions
1. I is once again con i med ha be o e he a i al o in e plane a y shocks a he Ea h’s o bi , in he
ine ial pa o he sola wind u bulence spec a in he equency ange ~10
-4
÷ 10
-2
Hz, FMS wa es o
signi ican ampli ude a e o en obse ed.
2. FMS wa es a e gene a ed by luxes o supe - he mal pa icles wi h ene gy Ep~1 MeV in he icini y o
he shock on .
3. The lux o galac ic CRs has been subjec o modula ion by FMS wa es, which mani es s i sel in cohe -
ence as he appea ance o signi ican CR luc ua ions a equencies ~10
-4
÷ 10
-2
Hz.
4. The esul s ob ained indica e he possibili y o de eloping and implemen ing in eal ime a me hod o
p edic ing s ong geophysical mani es a ions o space wea he based on g ound-based measu emen s
o CR in ensi y.
Acknowledgemen s
The wo k was ca ied ou wi hin he amewo k o he Russian Science Founda ion p ojec No. 22-22-
20045. The Yaku sk CR s a ions and Tixie Bay a e pa o he unique scien i ic acili y o he Russian
Fede a ion ‘Russian Ne wo k o Cosmic Ray G ound S a ions’ and NMDB.
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