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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2580 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ | 0.6735 | 0.8436 | 0.7984 | [M:[1.0886, 0.7343, 0.9621, 0.8607, 1.1393, 0.6836, 1.0886], q:[0.5443, 0.3671], qb:[0.4936, 0.7721], phi:[0.4557]] | [M:[[4], [-12], [-13], [5], [-5], [-3], [4]], q:[[2], [-6]], qb:[[11], [1]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{6}$, ${ }M_{2}$, ${ }M_{4}$, ${ }M_{3}$, ${ }M_{1}$, ${ }M_{7}$, ${ }M_{5}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{2}M_{6}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}M_{6}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}M_{6}$, ${ }M_{2}M_{3}$, ${ }M_{4}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{6}$, ${ }M_{6}M_{7}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{3}M_{4}$, ${ }M_{5}M_{6}$, ${ }M_{2}M_{7}$, ${ }M_{2}M_{5}$, ${ }M_{6}\phi_{1}q_{2}^{2}$, ${ }M_{3}^{2}$, ${ }M_{2}\phi_{1}q_{2}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}M_{7}$ | ${}M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ | -1 | t^2.051 + t^2.203 + t^2.582 + t^2.886 + 2*t^3.266 + t^3.418 + t^3.57 + t^3.949 + 2*t^4.101 + t^4.253 + t^4.329 + t^4.406 + t^4.481 + 2*t^4.633 + t^4.785 + t^4.937 + t^5.089 + t^5.164 + 2*t^5.316 + 3*t^5.469 + t^5.621 + 2*t^5.773 + t^5.848 - t^6. + 4*t^6.152 + 3*t^6.304 + 2*t^6.456 + 3*t^6.531 + t^6.608 + 3*t^6.684 + 3*t^6.836 + t^6.911 + 3*t^6.988 + 2*t^7.14 + t^7.215 + t^7.292 + 3*t^7.367 + 4*t^7.519 + t^7.594 + 4*t^7.671 + t^7.747 + 2*t^7.823 + t^7.899 + 2*t^7.975 + 2*t^8.203 + 5*t^8.355 + 3*t^8.507 + t^8.657 + 3*t^8.659 + 5*t^8.734 + t^8.809 + t^8.811 + t^8.962 - t^4.367/y - t^6.418/y - t^6.57/y + t^7.101/y + t^7.481/y + t^7.785/y + t^7.937/y + t^8.089/y + t^8.164/y + (3*t^8.316)/y + (3*t^8.469)/y + t^8.621/y + (2*t^8.848)/y - t^4.367*y - t^6.418*y - t^6.57*y + t^7.101*y + t^7.481*y + t^7.785*y + t^7.937*y + t^8.089*y + t^8.164*y + 3*t^8.316*y + 3*t^8.469*y + t^8.621*y + 2*t^8.848*y | t^2.051/g1^3 + t^2.203/g1^12 + g1^5*t^2.582 + t^2.886/g1^13 + 2*g1^4*t^3.266 + t^3.418/g1^5 + t^3.57/g1^14 + g1^3*t^3.949 + (2*t^4.101)/g1^6 + t^4.253/g1^15 + g1^20*t^4.329 + t^4.406/g1^24 + g1^11*t^4.481 + 2*g1^2*t^4.633 + t^4.785/g1^7 + t^4.937/g1^16 + t^5.089/g1^25 + g1^10*t^5.164 + 2*g1*t^5.316 + (3*t^5.469)/g1^8 + t^5.621/g1^17 + (2*t^5.773)/g1^26 + g1^9*t^5.848 - t^6. + (4*t^6.152)/g1^9 + (3*t^6.304)/g1^18 + (2*t^6.456)/g1^27 + 3*g1^8*t^6.531 + t^6.608/g1^36 + (3*t^6.684)/g1 + (3*t^6.836)/g1^10 + g1^25*t^6.911 + (3*t^6.988)/g1^19 + (2*t^7.14)/g1^28 + g1^7*t^7.215 + t^7.292/g1^37 + (3*t^7.367)/g1^2 + (4*t^7.519)/g1^11 + g1^24*t^7.594 + (4*t^7.671)/g1^20 + g1^15*t^7.747 + (2*t^7.823)/g1^29 + g1^6*t^7.899 + (2*t^7.975)/g1^38 + (2*t^8.203)/g1^12 + (5*t^8.355)/g1^21 + (3*t^8.507)/g1^30 + g1^40*t^8.657 + (3*t^8.659)/g1^39 + (5*t^8.734)/g1^4 + g1^31*t^8.809 + t^8.811/g1^48 + g1^22*t^8.962 - t^4.367/(g1^2*y) - t^6.418/(g1^5*y) - t^6.57/(g1^14*y) + t^7.101/(g1^6*y) + (g1^11*t^7.481)/y + t^7.785/(g1^7*y) + t^7.937/(g1^16*y) + t^8.089/(g1^25*y) + (g1^10*t^8.164)/y + (3*g1*t^8.316)/y + (3*t^8.469)/(g1^8*y) + t^8.621/(g1^17*y) + (2*g1^9*t^8.848)/y - (t^4.367*y)/g1^2 - (t^6.418*y)/g1^5 - (t^6.57*y)/g1^14 + (t^7.101*y)/g1^6 + g1^11*t^7.481*y + (t^7.785*y)/g1^7 + (t^7.937*y)/g1^16 + (t^8.089*y)/g1^25 + g1^10*t^8.164*y + 3*g1*t^8.316*y + (3*t^8.469*y)/g1^8 + (t^8.621*y)/g1^17 + 2*g1^9*t^8.848*y |
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 |
---|---|---|---|---|---|---|---|---|---|
1467 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}^{2}$ | 0.7129 | 0.8776 | 0.8123 | [M:[1.0543, 0.837, 0.8913, 1.0, 1.0, 0.8913, 1.0543], q:[0.5272, 0.4185], qb:[0.5815, 0.5815], phi:[0.4728]] | t^2.511 + 2*t^2.674 + 2*t^3. + 2*t^3.163 + t^3.93 + t^4.256 + 2*t^4.419 + t^4.581 + 2*t^4.744 + 3*t^4.907 + t^5.022 + 2*t^5.185 + 3*t^5.348 + 5*t^5.674 + 2*t^5.837 - 3*t^6. - t^4.419/y - t^4.419*y | detail |