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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55082 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ | 0.67 | 0.8476 | 0.7904 | [M:[0.7719, 1.1579, 0.8421, 0.8421, 0.7719, 0.7018], q:[0.8421, 0.386], qb:[0.4561, 0.7719], phi:[0.386]] | [M:[[2], [3], [-3], [-3], [2], [7]], q:[[-3], [1]], qb:[[-4], [2]], phi:[[1]]] | 1 | {a: 1935/2888, c: 306/361, M1: 44/57, M2: 22/19, M3: 16/19, M4: 16/19, M5: 44/57, M6: 40/57, q1: 16/19, q2: 22/57, qb1: 26/57, qb2: 44/57, phi1: 22/57} |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{6}$, ${ }M_{1}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{4}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{6}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}M_{4}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{6}\phi_{1}q_{2}^{2}$, ${ }M_{5}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}^{2}$, ${ }M_{6}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$ | ${}M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }M_{6}q_{1}\tilde{q}_{1}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ | 1 | t^2.105 + 3*t^2.316 + 2*t^2.526 + t^3.474 + t^3.684 + t^3.895 + t^4.211 + 3*t^4.421 + 8*t^4.632 + 7*t^4.842 + 3*t^5.053 + t^5.579 + 2*t^5.789 + t^6. + 3*t^6.211 + t^6.316 + 2*t^6.421 + 3*t^6.526 + 8*t^6.737 + 16*t^6.947 + 13*t^7.158 + 6*t^7.368 + 3*t^7.579 + t^7.684 + t^7.789 + 2*t^7.895 + t^8.105 - 4*t^8.316 + t^8.421 - 2*t^8.526 + 3*t^8.632 + 4*t^8.737 + 8*t^8.842 + 3*t^8.947 - t^4.158/y - t^6.263/y - (3*t^6.474)/y - t^6.684/y + (3*t^7.421)/y + (6*t^7.632)/y + (9*t^7.842)/y + (2*t^8.053)/y - t^8.368/y - (2*t^8.579)/y - (3*t^8.789)/y - t^4.158*y - t^6.263*y - 3*t^6.474*y - t^6.684*y + 3*t^7.421*y + 6*t^7.632*y + 9*t^7.842*y + 2*t^8.053*y - t^8.368*y - 2*t^8.579*y - 3*t^8.789*y | g1^7*t^2.105 + 3*g1^2*t^2.316 + (2*t^2.526)/g1^3 + g1^3*t^3.474 + t^3.684/g1^2 + t^3.895/g1^7 + g1^14*t^4.211 + 3*g1^9*t^4.421 + 8*g1^4*t^4.632 + (7*t^4.842)/g1 + (3*t^5.053)/g1^6 + g1^10*t^5.579 + 2*g1^5*t^5.789 + t^6. + (3*t^6.211)/g1^5 + g1^21*t^6.316 + (2*t^6.421)/g1^10 + 3*g1^16*t^6.526 + 8*g1^11*t^6.737 + 16*g1^6*t^6.947 + 13*g1*t^7.158 + (6*t^7.368)/g1^4 + (3*t^7.579)/g1^9 + g1^17*t^7.684 + t^7.789/g1^14 + 2*g1^12*t^7.895 + g1^7*t^8.105 - 4*g1^2*t^8.316 + g1^28*t^8.421 - (2*t^8.526)/g1^3 + 3*g1^23*t^8.632 + (4*t^8.737)/g1^8 + 8*g1^18*t^8.842 + (3*t^8.947)/g1^13 - (g1*t^4.158)/y - (g1^8*t^6.263)/y - (3*g1^3*t^6.474)/y - t^6.684/(g1^2*y) + (3*g1^9*t^7.421)/y + (6*g1^4*t^7.632)/y + (9*t^7.842)/(g1*y) + (2*t^8.053)/(g1^6*y) - (g1^15*t^8.368)/y - (2*g1^10*t^8.579)/y - (3*g1^5*t^8.789)/y - g1*t^4.158*y - g1^8*t^6.263*y - 3*g1^3*t^6.474*y - (t^6.684*y)/g1^2 + 3*g1^9*t^7.421*y + 6*g1^4*t^7.632*y + (9*t^7.842*y)/g1 + (2*t^8.053*y)/g1^6 - g1^15*t^8.368*y - 2*g1^10*t^8.579*y - 3*g1^5*t^8.789*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 |
---|---|---|---|---|---|---|---|---|---|
46910 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ | 0.6497 | 0.8094 | 0.8027 | [M:[0.7774, 1.166, 0.834, 0.834, 0.7774], q:[0.834, 0.3887], qb:[0.4453, 0.7774], phi:[0.3887]] | 3*t^2.332 + 2*t^2.502 + t^3.498 + t^3.668 + 2*t^3.838 + 6*t^4.664 + 7*t^4.834 + 3*t^5.004 + t^5.83 - t^4.166/y - t^4.166*y | detail |