Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
# | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
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46156 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}^{2}$ | 0.6484 | 0.7955 | 0.8151 | [M:[0.7076, 0.7005, 0.6981, 1.2971], q:[0.4717, 0.8207], qb:[0.8279, 0.474], phi:[0.3514]] | [M:[[8, -8], [-1, -5], [-4, -4], [-2, 6]], q:[[-3, 5], [-5, 3]], qb:[[4, 0], [0, 4]], phi:[[1, -3]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{3}$, ${ }M_{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}M_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$ | ${}$ | -2 | t^2.094 + t^2.101 + t^2.123 + t^2.837 + 2*t^3.884 + 2*t^3.891 + t^3.899 + t^4.189 + t^4.196 + t^4.203 + t^4.217 + t^4.224 + t^4.246 + t^4.931 + t^4.939 + t^4.946 + t^4.96 + t^5.674 + 2*t^5.979 + 3*t^5.986 + t^5.993 - 2*t^6. + t^6.014 + t^6.021 + t^6.283 + t^6.29 + t^6.297 + t^6.304 + t^6.311 + t^6.319 + t^6.326 + t^6.34 + t^6.347 + t^6.369 + 2*t^6.721 + 2*t^6.728 + t^6.736 + t^7.026 + t^7.033 + t^7.04 - t^7.047 - t^7.054 - t^7.061 + t^7.083 + 3*t^7.768 + 3*t^7.776 + 3*t^7.783 + t^7.797 + 2*t^8.073 + 3*t^8.08 + 2*t^8.087 - 2*t^8.094 - 2*t^8.101 + t^8.109 - 2*t^8.123 + t^8.137 + t^8.144 + t^8.377 + t^8.384 + t^8.391 + t^8.399 + 2*t^8.406 + t^8.413 + t^8.42 + t^8.427 + t^8.434 + t^8.442 + t^8.449 + t^8.463 + t^8.47 + t^8.492 + t^8.511 + 2*t^8.816 + 2*t^8.823 + t^8.83 - 2*t^8.837 - t^8.844 + t^8.859 - t^4.054/y - t^6.149/y - t^6.156/y - t^6.177/y + t^7.196/y + t^7.217/y + t^7.224/y + (2*t^7.931)/y + t^7.939/y + t^7.953/y + (2*t^7.96)/y - t^8.243/y - t^8.25/y - t^8.257/y - t^8.272/y - t^8.279/y - t^8.3/y + (2*t^8.979)/y + (4*t^8.986)/y + (3*t^8.993)/y - t^4.054*y - t^6.149*y - t^6.156*y - t^6.177*y + t^7.196*y + t^7.217*y + t^7.224*y + 2*t^7.931*y + t^7.939*y + t^7.953*y + 2*t^7.96*y - t^8.243*y - t^8.25*y - t^8.257*y - t^8.272*y - t^8.279*y - t^8.3*y + 2*t^8.979*y + 4*t^8.986*y + 3*t^8.993*y | t^2.094/(g1^4*g2^4) + t^2.101/(g1*g2^5) + (g1^8*t^2.123)/g2^8 + (g2^9*t^2.837)/g1^3 + (2*g2^7*t^3.884)/g1^5 + (2*g2^6*t^3.891)/g1^2 + g1*g2^5*t^3.899 + t^4.189/(g1^8*g2^8) + t^4.196/(g1^5*g2^9) + t^4.203/(g1^2*g2^10) + (g1^4*t^4.217)/g2^12 + (g1^7*t^4.224)/g2^13 + (g1^16*t^4.246)/g2^16 + (g2^5*t^4.931)/g1^7 + (g2^4*t^4.939)/g1^4 + (g2^3*t^4.946)/g1 + g1^5*g2*t^4.96 + (g2^18*t^5.674)/g1^6 + (2*g2^3*t^5.979)/g1^9 + (3*g2^2*t^5.986)/g1^6 + (g2*t^5.993)/g1^3 - 2*t^6. + (g1^6*t^6.014)/g2^2 + (g1^9*t^6.021)/g2^3 + t^6.283/(g1^12*g2^12) + t^6.29/(g1^9*g2^13) + t^6.297/(g1^6*g2^14) + t^6.304/(g1^3*g2^15) + t^6.311/g2^16 + (g1^3*t^6.319)/g2^17 + (g1^6*t^6.326)/g2^18 + (g1^12*t^6.34)/g2^20 + (g1^15*t^6.347)/g2^21 + (g1^24*t^6.369)/g2^24 + (2*g2^16*t^6.721)/g1^8 + (2*g2^15*t^6.728)/g1^5 + (g2^14*t^6.736)/g1^2 + (g2*t^7.026)/g1^11 + t^7.033/g1^8 + t^7.04/(g1^5*g2) - t^7.047/(g1^2*g2^2) - (g1*t^7.054)/g2^3 - (g1^4*t^7.061)/g2^4 + (g1^13*t^7.083)/g2^7 + (3*g2^14*t^7.768)/g1^10 + (3*g2^13*t^7.776)/g1^7 + (3*g2^12*t^7.783)/g1^4 + g1^2*g2^10*t^7.797 + (2*t^8.073)/(g1^13*g2) + (3*t^8.08)/(g1^10*g2^2) + (2*t^8.087)/(g1^7*g2^3) - (2*t^8.094)/(g1^4*g2^4) - (2*t^8.101)/(g1*g2^5) + (g1^2*t^8.109)/g2^6 - (2*g1^8*t^8.123)/g2^8 + (g1^14*t^8.137)/g2^10 + (g1^17*t^8.144)/g2^11 + t^8.377/(g1^16*g2^16) + t^8.384/(g1^13*g2^17) + t^8.391/(g1^10*g2^18) + t^8.399/(g1^7*g2^19) + (2*t^8.406)/(g1^4*g2^20) + t^8.413/(g1*g2^21) + (g1^2*t^8.42)/g2^22 + (g1^5*t^8.427)/g2^23 + (g1^8*t^8.434)/g2^24 + (g1^11*t^8.442)/g2^25 + (g1^14*t^8.449)/g2^26 + (g1^20*t^8.463)/g2^28 + (g1^23*t^8.47)/g2^29 + (g1^32*t^8.492)/g2^32 + (g2^27*t^8.511)/g1^9 + (2*g2^12*t^8.816)/g1^12 + (2*g2^11*t^8.823)/g1^9 + (g2^10*t^8.83)/g1^6 - (2*g2^9*t^8.837)/g1^3 - g2^8*t^8.844 + g1^6*g2^6*t^8.859 - (g1*t^4.054)/(g2^3*y) - t^6.149/(g1^3*g2^7*y) - t^6.156/(g2^8*y) - (g1^9*t^6.177)/(g2^11*y) + t^7.196/(g1^5*g2^9*y) + (g1^4*t^7.217)/(g2^12*y) + (g1^7*t^7.224)/(g2^13*y) + (2*g2^5*t^7.931)/(g1^7*y) + (g2^4*t^7.939)/(g1^4*y) + (g1^2*g2^2*t^7.953)/y + (2*g1^5*g2*t^7.96)/y - t^8.243/(g1^7*g2^11*y) - t^8.25/(g1^4*g2^12*y) - t^8.257/(g1*g2^13*y) - (g1^5*t^8.272)/(g2^15*y) - (g1^8*t^8.279)/(g2^16*y) - (g1^17*t^8.3)/(g2^19*y) + (2*g2^3*t^8.979)/(g1^9*y) + (4*g2^2*t^8.986)/(g1^6*y) + (3*g2*t^8.993)/(g1^3*y) - (g1*t^4.054*y)/g2^3 - (t^6.149*y)/(g1^3*g2^7) - (t^6.156*y)/g2^8 - (g1^9*t^6.177*y)/g2^11 + (t^7.196*y)/(g1^5*g2^9) + (g1^4*t^7.217*y)/g2^12 + (g1^7*t^7.224*y)/g2^13 + (2*g2^5*t^7.931*y)/g1^7 + (g2^4*t^7.939*y)/g1^4 + g1^2*g2^2*t^7.953*y + 2*g1^5*g2*t^7.96*y - (t^8.243*y)/(g1^7*g2^11) - (t^8.25*y)/(g1^4*g2^12) - (t^8.257*y)/(g1*g2^13) - (g1^5*t^8.272*y)/g2^15 - (g1^8*t^8.279*y)/g2^16 - (g1^17*t^8.3*y)/g2^19 + (2*g2^3*t^8.979*y)/g1^9 + (4*g2^2*t^8.986*y)/g1^6 + (3*g2*t^8.993*y)/g1^3 |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
# | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
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Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|---|
45957 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ | 0.6689 | 0.8347 | 0.8014 | [M:[0.7027, 0.6964, 0.6943], q:[0.4751, 0.8222], qb:[0.8285, 0.4772], phi:[0.3492]] | t^2.083 + t^2.089 + t^2.095 + t^2.108 + t^2.857 + 2*t^3.898 + t^3.905 + t^3.911 + t^4.166 + t^4.172 + 2*t^4.178 + t^4.185 + 2*t^4.191 + t^4.197 + t^4.203 + t^4.216 + t^4.94 + t^4.946 + 2*t^4.952 + t^4.965 + t^5.714 + 2*t^5.981 + 2*t^5.987 + 2*t^5.994 - t^6. - t^4.048/y - t^4.048*y | detail |