Dubna1mHBC he4p8
Ožiarenie 1m HBC zväzkami jadier 4He pri hybnosti 8,6 GeV/c
DODAT POPIS STUKTURY DST PRE FULL A MINI FORMAT
Expozície číslo: 40, 41 hybnosť zväzku 4He 8,6 GeV/c.Formaty DST plný (FULL) format a MINI format.
Vysvetlenie rozdielu medzi hypotezou a kanalom reakcie
Hypoteza pod danym cislom, ako je uvedena v zozname, moze zahrnut — v dosledku zakona zachovania elektrickeho naboja a baryonoveho cisla — niekolko kanalov reakcie :
- kanal bez neutralnej castice (4C-, 3C-, 2C-fit)
- kanal s 1 (jednou) neutralnou casticou (1C-fit)
- kanal s 2 (dvoma) a viac neutralnymi casticami (0C-fit tiez nazyvany ako NOFIT).
Pripad (event) moze obsahovat maximalne 2 (dve) hypotezy.
Plný format (FULL) binárny file
| File | Počet prípadov | Expozícia |
|---|---|---|
| he8p2p4.dvo | 13766 | 40, 41 |
| he8p3p5.dvo | 13185 | 40, 41 |
| he8pnfit.dvo | 11761 | 40, 41 |
| Total | 38712 | all |
Štruktúra zápisu
- Nbytes, Nwords, b[0], b[1], …, b[Nwords-1], Nbytes,
kde
- Nbytes je štvorbyteový integer a Nbytes = 4 * (Nwords + 1) dlžka zápisu v štvorbyteových slovách, samotné slová Nbytes sa do dl´žky nezapočítavajú,
- Nwords je štvorbyteový integer a vyjadruje dlžku poľa
- b[0], b[1], … b[Nwords-1], samotné slovo Nwords sa do dl´žky nezapočítavá,
- b[0], b[1], … b[Nwords-1] sú štvorbyteový integer alebo float,
- b[0], b[1] sú integer (pre lab Dubna, ostatné float)
- b[2], … b[Nwords-1] sú float
Čítanie: read Nbytes, Nwords ; read b[0], b[1], …, b[Nwords-1] ; read Nbytes
Podrobný popis štruktúry neskoršie.
Dĺžka hlavičky = 28; [0], …, [27]. Začiatok oblasti dráh = @ [29], length = 20/track, počet dráh = (SCANTOP/100 + 2)
Výsledky
Niektoré anomálie v NOFIT hypotézach:
- expozície 10 a 11 asi v polovine prípadov, inač ako má byť, spravna hodnota 40, 41 vysvetlenie bude neskorsie
- pre NOFIT cisla hypotez nie su zaporne
- pre NOFIT hypotezy ND nie je nulový 10332 hypo, NEPOUŽIŤ ND
- χ2 a PROB sú nenulové 765 hypo, pôvod neviem
- HYPO weight (W1 a W2) je nulový u 6239 hypo, NEPOUŽIŤ ich!
- Hmota neutralneho systemu je nulova v NOFIT hypotezach
- Tieto anomálie sú prítomné v každom LAB = 1, 2, 6
- Messy (chaotické) prípady:
- 2 hypotézy z nich jedna ma nulové číslo hypo (4 prípady) môže ísť aj o fit nofit konkurenciu? Track region vyzerá normálne.
- 1 hypotéza hlavička hytpotézy (info) sú samé nuly (10 prípadov)
- vylúčiť ich z analýzy ?
- POUŽíVAŤ iba váhu prípadu [9] a počet hypo [8], kde striktne plati [9] = 1/[8], vahy u hypotez [18] a [27] su nepochopitelne
- FITNOFIT flag je OK, na testovanie POUŽíVAŤ výhradne FITNOFIT flag
Anomálie prítomné vo všetkých hypotézach
- π- mezon má KLADNÚ hmotnosť !!!!! ????, mal by mať zápornú, bude asi vždy posledná nabitá častica
- Oblasť dráh obsahuje 20 slov, z nich 18 je užitočných, pre primarky PY=0 a PZ=0, posledné užitočné slovo je dĺžka dráhy (u primárky sa dobre identifikuje je záporna a má niekoľko desiatok cm). Slovo [18] a [19] neobsahuje vyuzitelnu informaciu. Boli dodane, aby oblast nasledujucej drahy zacal od okruhleho cisla.
- Za kazdou hypotezou a keď sú dve tak aj medzi nimi idú float čisla. Zmysel je, aby track region druhej hypotezy zacal od okruhleho cisla. To už vidieť aj z tabuľky krokov - vzdialenost medzi prvou a druhou hypotezou v zavislosti od poctu nabitych sekundarnych castic - je väčšia ako (Ntop+2) * trackregionlength:
// ? ? 2pr 3pr 4pr 5pr 6pr 7pr
int DELTA[] = { 0, 0, 100, 120, 160, 210, 270, 360};
- Z suradnica vertexu (-30, -9) cm OK a (0, 2) cm shifted beam -- Fig. 1., Lab vs VZ ==> vsetko posunutie je v Lab=6 -- Fig. 2.
- Hybnosti primarky su v ramci chyb rovnake pre Lab =1 , 2, 6 .
- Porovnal som fitted hybnost beam a measured p, λ a φ beam a secondaries v chamber systeme po laboratoriach - vizualne nevidiet rozdiel. Nechapem rozdiel v suradniciach vertexu :
- vertex je corresponding point,
- pozicia vertexu je upresnena minimalizaciou objemu, vytvoreneho pretinanim meranych velicin drah.
- Napriek tejto skutocnosti, mozeme data z Lab 6 zahrnut a pouzit MINI DST, pretoze:
- Vypis po 10 eventoch pre 60040 a 60041 ukazuje, ze VZ: je bud 0.5 alebo 1.
- Z histogramu Lab(y) vs Z Verte(x) pre Lab=6 -- Fig. 2. sa da vycitat, ze:
- VZ=0.5 pre 443 evts a
- VZ=1 pre 4493 evts,
- co sa zhoduje s celkovym poctom eventov 4936 pre Lab=6 -- Fig. 3..
- Cely problem bol vytvoreny umelo. Miesto VZ sa zapisal WEIGHT. Histo VZ vs WEIGHT pre Lab=6 -- Fig. 3. -- ukazuje obsah binu (WEIGHT=0.5, VZ=0.5) = 443 a binu (WEIGHT=1, VZ=1) = 4493 ostatne biny su prazdne.
Dodanie grind-checking kriterii na akceptovanie/zamietnutie hypotezy do analyzacneho macra (obecne pre celu DST):
- pravdepodobnost a ND je v hlavicke hypotezy su jednoducho spojene, vidiet z ND vs prob, ze toto kriterium (p > 0.001 pre 4,3 C a p> 0.05 pre 1C) nie je vzdy dodrzovane
- MMS je tiez v hlavicke, slabo zavisi od cisla hypotezy, da sa dodat, ale moze byt komplikovanejsie
- modul hybnosti castic treba vypocitat a preverit pre kazdu sekundarnu casticu
- a vsetky previerky treba robit v cykle cez pocet hypotez pred plnenim histogramu
- testovat konkretny vysledny kanal reakcie na dodrziavanie grind-checking kriterii je pohodlnejsie, preto to robit obecne NEidem
Zoznam filmov pre exp 40 a 41 z FULL DST
Exp 10
52 53 54 55 56 57
60 61 62 63
71
Exp 11
100 105
110 112 114 115 116 117
120
122 123 124 125 126 127
130 131 132 133 134 135 136 137
140 141 143 145 146
152 154 156 157
160 162 163 164 165
170 173 175
202
210 211 212 213 215
220 221 222 224 225 227
243 246 267
273 276 277
300 301 302 303 304 305 306 307 310
311 313 314
Exp 40
13 14 15 16
23 24 25 26
310
320 324
360
410
Exp 41
52 53 54 55 56 57
60 61 62 63
71
100 105
110 111 112 114 115 116 117
120 121 122 123 124 125 126 127 130
131 132 133 134 135 136 137
140 141 143 144 145 146 147
150 151 152 154 155 156 157
160 161 162 163 164 165 166 167
170 171 172 173 175
202
210 211 212 213 215 217
220 221 222 223 224 225 227
235 236 237
240 241 242 243 244 245 246 247 250
251 267 273 276 277
300 301 302 303 304 305 306 307 310
311 313 314
Nie vsetky prekryvajuce su vyznacene.
Ide o to, ze cast NOFIT hypotez v Lab=1 ma exp 10 resp 11.
|
|
|
660.25(Nofit exp10) + 4730.5(Nofit exp11) + 936.5(Nofit 40+41 Lab=1) = 6327.25(Lab=1 NOFIT)
Redukovaný format (MINI, MIKRO) binárny file
| File | Number of hypo | Exposition |
|---|---|---|
| he4prng2.dvo | 14483 | 40, 41 |
| he4prng3.dvo | 20692 | 40, 41 |
| he4prng4.dvo | 1336 | 40, 41 |
| he4prng5.dvo | 2174 | 40, 41 |
| Total | 38685 | all |
Štruktúra zápisu
- Nbytes, Nwords, b[0], b[1], …, b[Nwords-1], Nbytes,
kde
- Nbytes je štvorbyteový integer a Nbytes = 4 * (Nwords + 1) dlžka zápisu v štvorbyteových slovách, samotné slová Nbytes sa do dl´žky nezapočítavajú,
- Nwords je štvorbyteový integer a vyjadruje dlžku poľa, b[0], b[1], … b[Nwords-1], samotné slovo Nwords sa do dl´žky nezapočítavá,
- b[0], b[1] sú integer (pre lab Dubna, pre ostatne float )
- b[2], … b[Nwords-1] sú float
Čítanie: read Nbytes, Nwords ; read b[0], b[1], …, b[Nwords-1] ; read Nbytes
- Podrobný popis štruktúry neskoršie.
- Dĺžka hlavičky = 5 ( 0, …, 4)
- Začiatok oblasti dráh = @ [5], length = 6/track,
- scanning topology nie je na DST, počet dráh sa dá určiť takto: (Nwords – dĺžkahlavičky)/length/počethypotéz
- Cislovanie NOFIT hypotez je OK, < -100.5
Výsledky
Anomálie prítomné vo všetkých hypotézach
- π- mezon má KLADNÚ hmotnost, mal by mať zápornú, bude asi vždy posledná nabitá častica, pred neutralnou.
Zavery pre DST
- π- mezonu dat ZAPORNU hmotnost
- v NOFIT :
- zanulovat ND, CHISQ, PROBABILITY
- opravit cisla NOFIT hypo na < -100.5 (hlavne FULL DST)
- Lab=6 Z vertex = 0.5 resp 1 mozna sa da opravit (vypocitat), ale da sa s tym zit ako je
- rada pocas analyzy preverit grind checking kriteria pre hybnost a pravdepodobnost
Grind checking kriteria [math]\displaystyle{ ^{4}Hep }[/math] pri 8.6 GeV/c
- Pravdepodobnost P:
- 1C fit hypotez P > 0.05
- 2C fit hypotez P > 0.02
- 3C fit hypotez P > 0.005
- 4C fit hypotez P > 0.001
- Moduly laboratornych hybnosti p sekundarnych nabitych castic:
- [math]\displaystyle{ nabite \hspace{0.2cm} \pi \hspace{0.2cm} mezony \hspace{0.2cm} p_{\pi} \lt 3.0 GeV/c }[/math]
- [math]\displaystyle{ proton \hspace{0.2cm} p_{p} \lt 5.2 GeV/c }[/math]
- [math]\displaystyle{ deuteron \hspace{0.2cm} p_{d} \lt 5.2 GeV/c }[/math]
- [math]\displaystyle{ triton \hspace{0.2cm} p_{t} \gt 5.2 GeV/c }[/math]
- [math]\displaystyle{ ^{3}He \hspace{0.2cm} p_{^{3}He} \lt 7.2 GeV/c }[/math]
- [math]\displaystyle{ ^{4}He \hspace{0.2cm} p_{^{4}He} \gt 7.2 GeV/c }[/math]
- Kvadrat chybajucej hmotnosti pre 1C fit hypotez [math]\displaystyle{ MM^{2} }[/math]:
- s [math]\displaystyle{ \pi^{0} mezonom -0.2 \lt MM^{2}_{\pi^{0}} \lt 0.16 GeV^{2} }[/math]
- s neutronom [math]\displaystyle{ 0.4 \lt MM^{2}_{n} \lt 1.2 GeV^{2} }[/math]
- Kvadrat chybajucej hmotnosti pre NOFIT hypotez [math]\displaystyle{ MM^{2} }[/math]:
- s [math]\displaystyle{ X^{0}= k \pi^{0}, pre \hspace{0.2cm}k \gt 1, MM^{2}_{X^{0}} \gt 0.1 GeV^{2} }[/math]
- s [math]\displaystyle{ X^{0}= k \hspace{0.1cm} neutronov \hspace{0.2cm}(moze\hspace{0.1cm} obsahovat \hspace{0.1cm}\pi^{0}\hspace{0.1cm} mezon/y): }[/math]
- [math]\displaystyle{ pre \hspace{0.2cm}k = 1, MM^{2}_{X^{0}} \gt 1.17 GeV^{2} }[/math]
- [math]\displaystyle{ pre \hspace{0.2cm}k = 2, MM^{2}_{X^{0}} \gt 3.53 GeV^{2} }[/math]
- [math]\displaystyle{ pre \hspace{0.2cm}k = 3, MM^{2}_{X^{0}} \gt 7.94 GeV^{2} }[/math]
- [math]\displaystyle{ pre \hspace{0.2cm}k = 4, MM^{2}_{X^{0}} \gt 14.12 GeV^{2} }[/math]
- Pre FULL DST mozno pouzit vsetky 4 kriteria, ale pre bezne analyzy stacia 1,2,3.
- MINI DST umoznuje pouzit kriterium 2. Chybajuce hmotnosti sa daju dopocitat.
Navrh kodovania vystupnych kanalov reakcii iba pre exp. 40 & 41
- Pre kanaly bez neutralnej alebo s jednou neutralnou casticou :
- Pocet nabitych sekundarnych castic * 1000 + pocet neutralnych castic *100 + poradove cislo skupiny vystupneho kanalu ako je to v popise struktury DST.
- Pre kanaly obsahujuce dve a viac neutralnych castic : –(Pocet nabitych sekundarnych castic * 1000 + pocet neutralnych castic *100 + poradove cislo skupiny vystupneho kanalu), ako je to v popise struktury DST.Pre tieto kanaly neutralny system oznacujeme [math]\displaystyle{ X^{0} }[/math] a podla zakona zachovania baryonoveho cisla a energie reakcie moze obsahovat bud :
- dva a viac [math]\displaystyle{ \pi^{0} }[/math] alebo
- neutron a niekolko [math]\displaystyle{ \pi^{0} }[/math] alebo
- dva neutrony alebo
- dva neutron a niekolko [math]\displaystyle{ \pi^{0} }[/math] alebo
- tri neutrony alebo
- tri neutrony a niekolko [math]\displaystyle{ \pi^{0} }[/math].
| No neutral | One neutral | Two or more neutrals | ||||
| Kanal reakcie | Kod | Kanal reakcie | Kod | Kanal reakcie | [math]\displaystyle{ X^0 }[/math] | Kod |
| [math]\displaystyle{ ^4Hep \rightarrow {^4He}p }[/math] | 2001 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}p\pi^{0} }[/math] | 2101 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}pX^{0} }[/math] | [math]\displaystyle{ X^{0}=k\pi^0, k\ge2 }[/math] | -2101 |
| [math]\displaystyle{ ^4Hep \rightarrow {^3He}d }[/math] | 2002 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}d\pi^{0} }[/math] | 2102 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}dX^{0} }[/math] | [math]\displaystyle{ X^{0}=k\pi^0, k\ge2 }[/math] | -2102 |
| [math]\displaystyle{ ^4Hep \rightarrow {^3He}pn }[/math] | 2103 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}pX^{0} }[/math] | [math]\displaystyle{ X^{0}=n+k\pi^0, k\ge1 }[/math] | -2103 | ||
| [math]\displaystyle{ ^4Hep \rightarrow {^4He}\pi^+n }[/math] | 2104 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}\pi^+X^{0} }[/math] | [math]\displaystyle{ X^{0}=n+k\pi^0, k\ge1 }[/math] | -2104 | ||
| [math]\displaystyle{ ^4Hep \rightarrow {^3He}\pi^+X^{0} }[/math] | [math]\displaystyle{ X^{0}=2n+k\pi^0, k\ge0 }[/math] | -2105 | ||||
| [math]\displaystyle{ ^4Hep \rightarrow tpp }[/math] | 3001 | [math]\displaystyle{ ^4Hep \rightarrow tpp\pi^{0} }[/math] | 3101 | [math]\displaystyle{ ^4Hep \rightarrow tppX^{0} }[/math] | [math]\displaystyle{ X^{0}=k\pi^0, k\ge2 }[/math] | -3101 |
| [math]\displaystyle{ ^4Hep \rightarrow ddp }[/math] | 3002 | [math]\displaystyle{ ^4Hep \rightarrow ddp\pi^{0} }[/math] | 3102 | [math]\displaystyle{ ^4Hep \rightarrow ddpX^{0} }[/math] | [math]\displaystyle{ X^{0}=k\pi^0, k\ge2 }[/math] | -3102 |
| [math]\displaystyle{ ^4Hep \rightarrow td\pi^+ }[/math] | 3003 | [math]\displaystyle{ ^4Hep \rightarrow td\pi^+\pi^{0} }[/math] | 3103 | [math]\displaystyle{ ^4Hep \rightarrow td\pi^+X^{0} }[/math] | [math]\displaystyle{ X^{0}=k\pi^0, k\ge2 }[/math] | -3103 |
| [math]\displaystyle{ ^4Hep \rightarrow dppn }[/math] | 3104 | [math]\displaystyle{ ^4Hep \rightarrow dppX^{0} }[/math] | [math]\displaystyle{ X^{0}=n+k\pi^0, k\ge1 }[/math] | -3104 | ||
| [math]\displaystyle{ ^4Hep \rightarrow tp\pi^+n }[/math] | 3105 | [math]\displaystyle{ ^4Hep \rightarrow tp\pi^+X^{0} }[/math] | [math]\displaystyle{ X^{0}=n+k\pi^0, k\ge1 }[/math] | -3105 | ||
| [math]\displaystyle{ ^4Hep \rightarrow dd\pi^+n }[/math] | 3106 | [math]\displaystyle{ ^4Hep \rightarrow dd\pi^+X^{0} }[/math] | [math]\displaystyle{ X^{0}=n+k\pi^0, k\ge1 }[/math] | -3106 | ||
| [math]\displaystyle{ ^4Hep \rightarrow pppX^{0} }[/math] | [math]\displaystyle{ X^{0}=2n+k\pi^0, k\ge0 }[/math] | -3107 | ||||
| [math]\displaystyle{ ^4Hep \rightarrow t\pi^+\pi^+X^{0} }[/math] | [math]\displaystyle{ X^{0}=2n+k\pi^0, k\ge0 }[/math] | -3108 | ||||
| [math]\displaystyle{ ^4Hep \rightarrow dp\pi^+X^{0} }[/math] | [math]\displaystyle{ X^{0}=2n+k\pi^0, k\ge0 }[/math] | -3109 | ||||
| [math]\displaystyle{ ^4Hep \rightarrow d\pi^+\pi^+X^{0} }[/math] | [math]\displaystyle{ X^{0}=3n+k\pi^0, k\ge0 }[/math] | -3110 | ||||
| [math]\displaystyle{ ^4Hep \rightarrow pp\pi^+X^{0} }[/math] | [math]\displaystyle{ X^{0}=3n+k\pi^0, k\ge0 }[/math] | -3111 | ||||
| [math]\displaystyle{ ^4Hep \rightarrow p\pi^+\pi^+X^{0} }[/math] | [math]\displaystyle{ X^{0}=4n+k\pi^0, k\ge0 }[/math] | -3112 | ||||
| [math]\displaystyle{ ^4Hep \rightarrow \pi^+\pi^+\pi^+X^{0} }[/math] | [math]\displaystyle{ X^{0}=5n+k\pi^0, k\ge0 }[/math] | -3113 | ||||
| [math]\displaystyle{ ^4Hep \rightarrow {^3He}pp\pi^- }[/math] | 4001 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}pp\pi^-\pi^{0} }[/math] | 4101 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}pp\pi^-X^{0} }[/math] | [math]\displaystyle{ X^{0}=k\pi^0, k\ge2 }[/math] | -4101 |
| [math]\displaystyle{ ^4Hep \rightarrow {^4He}p\pi^+\pi^- }[/math] | 4002 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}p\pi^+\pi^-\pi^{0} }[/math] | 4102 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}p\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^{0}=k\pi^0, k\ge2 }[/math] | -4102 |
| [math]\displaystyle{ ^4Hep \rightarrow {^3He}d\pi^+\pi^- }[/math] | 4003 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}d\pi^+\pi^-\pi^{0} }[/math] | 4103 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}d\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^{0}=k\pi^0, k\ge2 }[/math] | -4103 |
| [math]\displaystyle{ ^4Hep \rightarrow {^3He}p\pi^+\pi^-n }[/math] | 4104 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}p\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^{0}=n+k\pi^0, k\ge1 }[/math] | -4104 | ||
| [math]\displaystyle{ ^4Hep \rightarrow {^4He}\pi^+\pi^+\pi^-n }[/math] | 4105 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}\pi^+\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^{0}=n+k\pi^0, k\ge1 }[/math] | -4105 | ||
| [math]\displaystyle{ ^4Hep \rightarrow {^3He}\pi^+\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^{0}=2n+k\pi^0, k\ge0 }[/math] | -4106 | ||||
| [math]\displaystyle{ ^4Hep \rightarrow td\pi^+\pi^+\pi^- }[/math] | 5001 | [math]\displaystyle{ ^4Hep \rightarrow td\pi^+\pi^+\pi^-\pi^{0} }[/math] | 5101 | [math]\displaystyle{ ^4Hep \rightarrow td\pi^+\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^{0}=k\pi^0, k\ge2 }[/math] | -5101 |
| [math]\displaystyle{ ^4Hep \rightarrow tpp\pi^+\pi^- }[/math] | 5002 | [math]\displaystyle{ ^4Hep \rightarrow tpp\pi^+\pi^-\pi^{0} }[/math] | 5102 | [math]\displaystyle{ ^4Hep \rightarrow tpp\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^{0}=k\pi^0, k\ge2 }[/math] | -5102 |
| [math]\displaystyle{ ^4Hep \rightarrow ddp\pi^+\pi^- }[/math] | 5003 | [math]\displaystyle{ ^4Hep \rightarrow ddp\pi^+\pi^-\pi^{0} }[/math] | 5103 | [math]\displaystyle{ ^4Hep \rightarrow ddp\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^{0}=k\pi^0, k\ge2 }[/math] | -5103 |
| [math]\displaystyle{ ^4Hep \rightarrow dppp\pi^- }[/math] | 5004 | [math]\displaystyle{ ^4Hep \rightarrow dppp\pi^-\pi^{0} }[/math] | 5104 | [math]\displaystyle{ ^4Hep \rightarrow dppp\pi^-X^{0} }[/math] | [math]\displaystyle{ X^{0}=k\pi^0, k\ge2 }[/math] | -5104 |
| [math]\displaystyle{ ^4Hep \rightarrow tp\pi^+\pi^+\pi^-n }[/math] | 5105 | [math]\displaystyle{ ^4Hep \rightarrow tp\pi^+\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^{0}=n+k\pi^0, k\ge1 }[/math] | -5105 | ||
| [math]\displaystyle{ ^4Hep \rightarrow dd\pi^+\pi^+\pi^-n }[/math] | 5106 | [math]\displaystyle{ ^4Hep \rightarrow dd\pi^+\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^{0}=n+k\pi^0, k\ge1 }[/math] | -5106 | ||
| [math]\displaystyle{ ^4Hep \rightarrow dpp\pi^+\pi^-n }[/math] | 5107 | [math]\displaystyle{ ^4Hep \rightarrow dpp\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^{0}=n+k\pi^0, k\ge1 }[/math] | -5107 | ||
| [math]\displaystyle{ ^4Hep \rightarrow pppp\pi^-n }[/math] | 5108 | [math]\displaystyle{ ^4Hep \rightarrow pppp\pi^-X^{0} }[/math] | [math]\displaystyle{ X^{0}=n+k\pi^0, k\ge1 }[/math] | -5108 | ||
| [math]\displaystyle{ ^4Hep \rightarrow dp\pi^+\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^{0}=2n+k\pi^0, k\ge0 }[/math] | -5109 | ||||
| [math]\displaystyle{ ^4Hep \rightarrow ppp\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^{0}=2n+k\pi^0, k\ge0 }[/math] | -5110 | ||||
| [math]\displaystyle{ ^4Hep \rightarrow pp\pi^+\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^{0}=3n+k\pi^0, k\ge0 }[/math] | -5111 | ||||
| [math]\displaystyle{ ^4Hep \rightarrow {^3He}pp\pi^+\pi^-\pi^- }[/math] | 6001 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}pp\pi^+\pi^-\pi^-\pi^{0} }[/math] | 6101 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}pp\pi^+\pi^-\pi^-X^{0} }[/math] | [math]\displaystyle{ X^{0}=k\pi^0, k\ge2 }[/math] | -6101 |
| [math]\displaystyle{ ^4Hep \rightarrow {^4He}p\pi^+\pi^+\pi^-\pi^- }[/math] | 6002 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}p\pi^+\pi^+\pi^-\pi^-\pi^{0} }[/math] | 6102 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}p\pi^+\pi^+\pi^-\pi^-X^{0} }[/math] | [math]\displaystyle{ X^{0}=k\pi^0, k\ge2 }[/math] | -6102 |
| [math]\displaystyle{ ^4Hep \rightarrow {^3He}d\pi^+\pi^+\pi^-\pi^- }[/math] | 6003 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}d\pi^+\pi^+\pi^-\pi^-\pi^{0} }[/math] | 6103 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}d\pi^+\pi^+\pi^-\pi^-X^{0} }[/math] | [math]\displaystyle{ X^{0}=k\pi^0, k\ge2 }[/math] | -6103 |
| [math]\displaystyle{ ^4Hep \rightarrow {^3He}p\pi^+\pi^+\pi^-\pi^-n }[/math] | 6104 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}p\pi^+\pi^+\pi^-\pi^-X^{0} }[/math] | [math]\displaystyle{ X^{0}=n+k\pi^0, k\ge1 }[/math] | -6104 | ||
| [math]\displaystyle{ ^4Hep \rightarrow {^4He}\pi^+\pi^+\pi^+\pi^-\pi^-n }[/math] | 6105 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}\pi^+\pi^+\pi^+\pi^-\pi^-X^{0} }[/math] | [math]\displaystyle{ X^{0}=n+k\pi^0, k\ge1 }[/math] | -6105 | ||
Cervena farba znamena narusenie poradia hypotez (=kanalov reakcie) voci pisomnemu zoznamu.
interna tab
| Por. | HYP od ÷ do | Kod reakcie | Nove | Kanal reakcie |
|---|---|---|---|---|
| 1. | 1 ÷ 12 | 6001 | 6101 | -6101 | 1 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}pp\pi^+\pi^-\pi^-| \pi^{0} | X^{0}, X^{0}= k\pi^{0}, k\ge2 }[/math] |
| 2. | 13 ÷ 24 | 6002 | 6102 | -6102 | 2 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}p\pi^+\pi^+\pi^-\pi^-| \pi^{0} | X^{0}, X^{0}= k\pi^{0}, k\ge2 }[/math] |
| 3. | 125 ÷ 136 | 6104 | -6104 | 4 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}p\pi^+\pi^+\pi^-\pi^-| n |X^{0}, X^{0}= n+k\pi^{0}, k\ge1 }[/math] |
| 4. | 37 ÷ 48 | 6003 | 6103 | -6103 | 3 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}d\pi^+\pi^+\pi^-\pi^-| \pi^{0} | X^{0}, X^{0}= k\pi^{0}, k\ge2 }[/math] |
| 5 | 149 ÷ 152 | 6105 | -6105 | 5 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}\pi^+\pi^+\pi^+\pi^-\pi^{-} | n | X^{0}, X^{0}= n+k\pi^{0}, k\ge1 }[/math] |
Prechod ku kodom [math]\displaystyle{ ^{4}Hep }[/math] pri 8.6 GeV/c (exp. 40&41) MINI format
| NHYP | KOD | Kanal reakcie | |
| 1 ≤ NHYP ≤ 2 | 2001 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}p }[/math] | |
| 101 ≤ NHYP ≤102 | 2101 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}\pi^{0} }[/math] | |
| -102 ≤ NHYP ≤ -101 | -2101 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}pX^{0} }[/math] | [math]\displaystyle{ X^0=k\pi^{0}, k\ge2 }[/math] |
| 3 ≤ NHYP ≤ 4 | 2002 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}d }[/math] | |
| 103 ≤ NHYP ≤ 104 | 2102 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}d\pi^{0} }[/math] | |
| -104 ≤ NHYP ≤ -103 | -2102 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}dX^{0} }[/math] | [math]\displaystyle{ X^0=k\pi^{0}, k\ge2 }[/math] |
| 105 ≤ NHYP ≤ 106 | 2103 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}pn }[/math] | |
| -106 ≤ NHYP ≤ -105 | -2103 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}pX^{0} }[/math] | [math]\displaystyle{ X^0=n+k\pi^{0}, k\ge1 }[/math] |
| 107 ≤ NHYP ≤ 108 | 2104 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}\pi^+n }[/math] | |
| -108 ≤ NHYP ≤ -107 | -2104 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}\pi^+X^{0} }[/math] | [math]\displaystyle{ X^0=n+k\pi^{0}, k\ge1 }[/math] |
| -110 ≤ NHYP ≤ -109 | -2105 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}\pi^+X^{0} }[/math] | [math]\displaystyle{ X^0=2n+k\pi^{0}, k\ge0 }[/math] |
| NHYP | KOD | Kanal reakcie | |
| 1 ≤ NHYP ≤ 3 | 4001 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}pp\pi^- }[/math] | |
| 101 ≤ NHYP ≤ 103 | 4101 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}pp\pi^-\pi^{0} }[/math] | |
| -103 ≤ NHYP ≤ -101 | -4101 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}pp\pi^-X^{0} }[/math] | [math]\displaystyle{ X^0=k\pi^{0}, k\ge2 }[/math] |
| 4 ≤ NHYP ≤ 9 | 4002 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}p\pi^+\pi^- }[/math] | |
| 104 ≤ NHYP ≤ 109 | 4102 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}p\pi^+\pi^-\pi^{0} }[/math] | |
| -109 ≤ NHYP ≤ -104 | -4102 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}p\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^0=k\pi^{0}, k\ge2 }[/math] |
| 10 ≤ NHYP ≤15 | 4003 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}d\pi^+\pi^- }[/math] | |
| 110 ≤ NHYP ≤115 | 4103 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}d\pi^+\pi^-\pi^{0} }[/math] | |
| -115 ≤ NHYP ≤ -110 | -4103 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}d\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^0=k\pi^{0}, k\ge2 }[/math] |
| 116 ≤ NHYP ≤ 121 | 4104 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}p\pi^+\pi^-n }[/math] | |
| -121 ≤ NHYP ≤ 116 | -4104 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}p\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^0=n+k\pi^{0}, k\ge1 }[/math] |
| 122 ≤ NHYP ≤ 124 | 4105 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}\pi^+\pi^+\pi^{-}n }[/math] | |
| -124 ≤ NHYP ≤ -122 | -4105 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}\pi^+\pi^+\pi^{-}X^{0} }[/math] | [math]\displaystyle{ X^0=n+k\pi^{0}, k\ge1 }[/math] |
| -127 ≤ NHYP ≤ -125 | -4106 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}\pi^+\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^0=2n+k\pi^{0}, k\ge0 }[/math] |
| NHYP | KOD | Kanal reakcie | |
| 1 ≤ NHYP ≤ 3 | 3001 | [math]\displaystyle{ ^4Hep \rightarrow tpp }[/math] | |
| 101 NHYP ≤103 | 3101 | [math]\displaystyle{ ^4Hep \rightarrow tpp\pi^{0} }[/math] | |
| -103 NHYP ≤ -101 | -3101 | [math]\displaystyle{ ^4Hep\rightarrow tppX^{0} }[/math] | [math]\displaystyle{ X^0=k\pi^{0}, k\ge2 }[/math] |
| 4 ≤ NHYP ≤ 6 | 3002 | [math]\displaystyle{ ^4Hep \rightarrow ddp }[/math] | |
| 104 ≤ NHYP ≤ 106 | 3102 | [math]\displaystyle{ ^4Hep \rightarrow ddp\pi^{0} }[/math] | |
| -106 ≤ NHYP ≤ -104 | -3102 | [math]\displaystyle{ ^4Hep \rightarrow ddpX^{0} }[/math] | [math]\displaystyle{ X^0=k\pi^{0}, k\ge2 }[/math] |
| 7 ≤ NHYP ≤ 12 | 3003 | [math]\displaystyle{ ^4Hep \rightarrow td\pi^+ }[/math] | |
| 107≤ NHYP ≤ 112 | 3103 | [math]\displaystyle{ ^4Hep \rightarrow td\pi^+\pi^{0} }[/math] | |
| -112 ≤ NHYP ≤ -107 | -3103 | [math]\displaystyle{ ^4Hep \rightarrow td\pi^+X^{0} }[/math] | [math]\displaystyle{ X^0=k\pi^{0}, k\ge2 }[/math] |
| 113 ≤ NHYP ≤ 115 | 3104 | [math]\displaystyle{ ^4Hep \rightarrow dppn }[/math] | |
| -115 ≤ NHYP ≤ -113 | -3104 | [math]\displaystyle{ ^4Hep \rightarrow dppX^{0} }[/math] | [math]\displaystyle{ X^0=n+k\pi^{0}, k\ge1 }[/math] |
| 116 ≤ NHYP ≤ 121 | 3105 | [math]\displaystyle{ ^4Hep \rightarrow tp\pi^+n }[/math] | |
| -121 ≤ NHYP ≤ -116 | -3105 | [math]\displaystyle{ ^4Hep \rightarrow tp\pi^+X^{0} }[/math] | [math]\displaystyle{ X^0=n+k\pi^{0}, k\ge1 }[/math] |
| 122 ≤ NHYP ≤ 124 | 3106 | [math]\displaystyle{ ^4Hep \rightarrow dd\pi^+n }[/math] | |
| -124 ≤ NHYP ≤ -122 | -3106 | [math]\displaystyle{ ^4Hep \rightarrow dd\pi^+X^{0} }[/math] | [math]\displaystyle{ X^0=n+k\pi^{0}, k\ge1 }[/math] |
| NHYP = -125 | -3107 | [math]\displaystyle{ ^4Hep \rightarrow pppX^{0} }[/math] | [math]\displaystyle{ X^0=2n+k\pi^{0}, k\ge0 }[/math] |
| -128 ≤ NHYP ≤ -126 | -3108 | [math]\displaystyle{ ^4Hep \rightarrow t\pi^+\pi^+X^{0} }[/math] | [math]\displaystyle{ X^0=2n+k\pi^{0}, k\ge0 }[/math] |
| -134 ≤ NHYP ≤ -129 | -3109 | [math]\displaystyle{ ^4Hep \rightarrow dp\pi^+X^{0} }[/math] | [math]\displaystyle{ X^0=2n+k\pi^{0}, k\ge0 }[/math] |
| -137 ≤ NHYP ≤ -135 | -3110 | [math]\displaystyle{ ^4Hep \rightarrow d\pi^+\pi^+X^{0} }[/math] | [math]\displaystyle{ X^0=3n+k\pi^{0}, k\ge0 }[/math] |
| -140 ≤ NHYP ≤ -138 | -3111 | [math]\displaystyle{ ^4Hep \rightarrow pp\pi^+X^{0} }[/math] | [math]\displaystyle{ X^0=3n+k\pi^{0}, k\ge0 }[/math] |
| -143 ≤ NHYP ≤ -141 | -3112 | [math]\displaystyle{ ^4Hep \rightarrow p\pi^+\pi^+X^{0} }[/math] | [math]\displaystyle{ X^0=4n+k\pi^{0}, k\ge0 }[/math] |
| NHYP = -144 | -3113 | [math]\displaystyle{ ^4Hep \rightarrow \pi^+\pi^+\pi^+X^{0} }[/math] | [math]\displaystyle{ X^0=5n+k\pi^{0}, k\ge0 }[/math] |
| NHYP | KOD | Kanal reakcie | |
| 41 ≤ NHYP ≤ 52 | 5001 | [math]\displaystyle{ ^4Hep \rightarrow td\pi^+\pi^+\pi^- }[/math] | |
| 141 ≤ NHYP ≤ 152 | 5101 | [math]\displaystyle{ ^4Hep \rightarrow td\pi^+\pi^+\pi^-\pi^{0} }[/math] | |
| -152 ≤ NHYP ≤ -141 | -5101 | [math]\displaystyle{ ^4Hep \rightarrow td\pi^+\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^0=k\pi^{0}, k\ge2 }[/math] |
| 1 ≤ NHYP ≤ 12 | 5002 | [math]\displaystyle{ ^4Hep \rightarrow tpp\pi^+\pi^- }[/math] | |
| 101 ≤ NHYP ≤ 112 | 5102 | [math]\displaystyle{ ^4Hep \rightarrow tpp\pi^+\pi^-\pi^{0} }[/math] | |
| -112 ≤ NHYP ≤ -101 | -5102 | [math]\displaystyle{ ^4Hep \rightarrow tpp\pi^+\pi^-X^{0} }[/math] | |
| 13 ≤ NHYP ≤ 24 | 5003 | [math]\displaystyle{ ^4Hep \rightarrow ddp\pi^+\pi^- }[/math] | |
| 113 ≤ NHYP ≤124 | 5103 | [math]\displaystyle{ ^4Hep \rightarrow ddp\pi^+\pi^-\pi^{0} }[/math] | |
| -124 ≤ NHYP ≤ -113 | -5103 | [math]\displaystyle{ ^4Hep \rightarrow ddp\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^0=k\pi^{0}, k\ge2 }[/math] |
| 37 ≤ NHYP ≤ 40 | 5004 | [math]\displaystyle{ ^4Hep \rightarrow dppp\pi^- }[/math] | |
| 137 ≤ NHYP ≤ 140 | 5104 | [math]\displaystyle{ ^4Hep \rightarrow dppp\pi^-\pi^{0} }[/math] | |
| -140 ≤ NHYP ≤ -137 | -5104 | [math]\displaystyle{ ^4Hep \rightarrow dppp\pi^-X^{0} }[/math] | [math]\displaystyle{ X^0=k\pi^{0}, k\ge2 }[/math] |
| 176 ≤ NHYP ≤ 187 | 5105 | [math]\displaystyle{ ^4Hep \rightarrow tp\pi^+\pi^+\pi^-n }[/math] | |
| -187 ≤ NHYP ≤-176 | -5105 | [math]\displaystyle{ ^4Hep \rightarrow tp\pi^+\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^0=n+k\pi^{0}, k\ge1 }[/math] |
| 188 ≤ NHYP ≤ 193 | 5106 | [math]\displaystyle{ ^4Hep \rightarrow dd\pi^+\pi^+\pi^-n }[/math] | |
| -193 ≤ NHYP ≤ -188 | -5106 | [math]\displaystyle{ ^4Hep \rightarrow dd\pi^+\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^0=n+k\pi^{0}, k\ge1 }[/math] |
| 125 ≤ NHYP ≤ 136 | 5107 | [math]\displaystyle{ ^4Hep \rightarrow dpp\pi^+\pi^-n }[/math] | |
| -136 ≤ NHYP ≤ -125 | -5107 | [math]\displaystyle{ ^4Hep \rightarrow dpp\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^0=n+k\pi^{0}, k\ge1 }[/math] |
| NHYP = 153 | 5108 | [math]\displaystyle{ ^4Hep \rightarrow pppp\pi^-n }[/math] | |
| NHYP = -153 | -5108 | [math]\displaystyle{ ^4Hep \rightarrow pppp\pi^-X^{0} }[/math] | [math]\displaystyle{ X^0=n+k\pi^{0}, k\ge1 }[/math] |
| -165 ≤ NHYP ≤ -154 | -5109 | [math]\displaystyle{ ^4Hep \rightarrow dp\pi^+\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^0=2n+k\pi^{0}, k\ge0 }[/math] |
| -175 ≤ NHYP ≤ -172 | -5110 | [math]\displaystyle{ ^4Hep \rightarrow ppp\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^0=2n+k\pi^{0}, k\ge0 }[/math] |
| -171 ≤ NHYP ≤ -166 | -5111 | [math]\displaystyle{ ^4Hep \rightarrow pp\pi^+\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^0=3n+k\pi^{0}, k\ge0 }[/math] |
| -197 ≤ NHYP ≤ -194 | -5112 | [math]\displaystyle{ ^4Hep \rightarrow t\pi^+\pi^+\pi^+\pi^-X^{0} }[/math] | [math]\displaystyle{ X^0=2n+k\pi^{0}, k\ge0 }[/math] |
Doplnenie k 5 lucovym kanalom: farebne vyznacene kanaly reakcie 5 lucovych (predosla a nasledujuca tabulka), celkom 6 (sest) hypotez, nie su uvedene v MINI DST zozname hypotez (exp 40&41), su ale v povodnom plnom zozname (iba pisomne). Plny zoznam (exp 40&41) obsahuje tri hypotezy (kanaly) reakcie naviac, aj v porovnani s plnym zoznamom hypotez pre exp. 42&43 4Hep pri 13.5 GeV/c, s nasledujucimi cislami:
| NHYP | Kanal reakcie |
|---|---|
| 94 ÷ 97 | [math]\displaystyle{ ^4Hep \rightarrow t\pi^+\pi^+\pi^+\pi^-X^{0}, X^0=2n+k\pi^{0}, k\ge0 }[/math] |
| 98 ÷ 101 | [math]\displaystyle{ ^4Hep \rightarrow d\pi^+\pi^+\pi^+\pi^-X^{0}, X^0=3n+k\pi^{0}, k\ge0 }[/math] |
| 102 ÷ 106 | [math]\displaystyle{ ^4Hep \rightarrow p\pi^+\pi^+\pi^+\pi^-X^{0}, X^0=4n+k\pi^{0}, k\ge0 }[/math] |
Na FULL DST sa kanaly s cislami hypotez nad 175 sa nevyskytuju, ako vidiet z rozdelenia hypotez na obrazku Fig. 4.
| NHYP | KOD | Kanal reakcie | |
| 1 ≤ NHYP ≤ 12 | 6001 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}pp\pi^+\pi^-\pi^- }[/math] | |
| 101 ≤ NHYP ≤ 112 | 6101 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}pp\pi^+\pi^-\pi^-\pi^{0} }[/math] | |
| -112 ≤ NHYP ≤-101 | -6101 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}pp\pi^+\pi^-\pi^-X^{0} }[/math] | [math]\displaystyle{ X^0=k\pi^{0}, k\ge2 }[/math] |
| 13 ≤ NHYP ≤ 24 | 6002 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}p\pi^+\pi^+\pi^-\pi^- }[/math] | |
| 113 ≤ NHYP ≤ 124 | 6102 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}p\pi^+\pi^+\pi^-\pi^-\pi^{0} }[/math] | |
| -124 ≤ NHYP ≤ -113 | -6102 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}p\pi^+\pi^+\pi^-\pi^-X^{0} }[/math] | [math]\displaystyle{ X^0=k\pi^{0}, k\ge2 }[/math] |
| 37 ≤ NHYP ≤ 48 | 6003 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}d\pi^+\pi^+\pi^-\pi^- }[/math] | |
| 137 ≤ NHYP ≤ 148 | 6103 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}d\pi^+\pi^+\pi^-\pi^-\pi^{0} }[/math] | |
| -148 ≤ NHYP ≤ -137 | -6103 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}d\pi^+\pi^+\pi^-\pi^-X^{0} }[/math] | [math]\displaystyle{ X^0=k\pi^{0}, k\ge2 }[/math] |
| 125 ≤ NHYP ≤ 136 | 6104 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}p\pi^+\pi^+\pi^-\pi^-n }[/math] | |
| -136 ≤ NHYP ≤-125 | -6104 | [math]\displaystyle{ ^4Hep \rightarrow {^3He}p\pi^+\pi^+\pi^-\pi^-X^{0} }[/math] | [math]\displaystyle{ X^0=n+k\pi^{0}, k\ge1 }[/math] |
| 149 ≤ NHYP ≤ 152 | 6105 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}\pi^+\pi^+\pi^+\pi^-\pi^-n }[/math] | |
| -152 ≤ NHYP ≤ -149 | -6105 | [math]\displaystyle{ ^4Hep \rightarrow {^4He}\pi^+\pi^+\pi^+\pi^-\pi^-X^{0} }[/math] | [math]\displaystyle{ X^0=n+k\pi^{0}, k\ge1 }[/math] |
