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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2324 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{6}X_{1}$ | 0.67 | 0.8476 | 0.7904 | [X:[1.614], M:[0.7719, 0.8421, 0.7018, 1.1579, 0.7719, 0.386, 0.8421], q:[0.7719, 0.4561], qb:[0.386, 0.8421], phi:[0.386]] | [X:[[1]], M:[[-2], [3], [-7], [-3], [-2], [-1], [3]], q:[[-2], [4]], qb:[[-1], [3]], phi:[[-1]]] | 1 | {a: 1935/2888, c: 306/361, X1: 92/57, M1: 44/57, M2: 16/19, M3: 40/57, M4: 22/19, M5: 44/57, M6: 22/57, M7: 16/19, q1: 44/57, q2: 26/57, qb1: 22/57, qb2: 16/19, phi1: 22/57} |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{3}$, ${ }M_{1}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{7}$, ${ }M_{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{3}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}M_{5}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{1}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{3}M_{7}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{5}$, ${ }M_{1}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{7}$, ${ }M_{7}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}M_{4}$, ${ }M_{1}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ | ${}M_{4}M_{7}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ | 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 | t^2.105/g1^7 + (3*t^2.316)/g1^2 + 2*g1^3*t^2.526 + t^3.474/g1^3 + g1^2*t^3.684 + g1^7*t^3.895 + t^4.211/g1^14 + (3*t^4.421)/g1^9 + (8*t^4.632)/g1^4 + 7*g1*t^4.842 + 3*g1^6*t^5.053 + t^5.579/g1^10 + (2*t^5.789)/g1^5 + t^6. + 3*g1^5*t^6.211 + t^6.316/g1^21 + 2*g1^10*t^6.421 + (3*t^6.526)/g1^16 + (8*t^6.737)/g1^11 + (16*t^6.947)/g1^6 + (13*t^7.158)/g1 + 6*g1^4*t^7.368 + 3*g1^9*t^7.579 + t^7.684/g1^17 + g1^14*t^7.789 + (2*t^7.895)/g1^12 + t^8.105/g1^7 - (4*t^8.316)/g1^2 + t^8.421/g1^28 - 2*g1^3*t^8.526 + (3*t^8.632)/g1^23 + 4*g1^8*t^8.737 + (8*t^8.842)/g1^18 + 3*g1^13*t^8.947 - t^4.158/(g1*y) - t^6.263/(g1^8*y) - (3*t^6.474)/(g1^3*y) - (g1^2*t^6.684)/y + (3*t^7.421)/(g1^9*y) + (6*t^7.632)/(g1^4*y) + (9*g1*t^7.842)/y + (2*g1^6*t^8.053)/y - t^8.368/(g1^15*y) - (2*t^8.579)/(g1^10*y) - (3*t^8.789)/(g1^5*y) - (t^4.158*y)/g1 - (t^6.263*y)/g1^8 - (3*t^6.474*y)/g1^3 - g1^2*t^6.684*y + (3*t^7.421*y)/g1^9 + (6*t^7.632*y)/g1^4 + 9*g1*t^7.842*y + 2*g1^6*t^8.053*y - (t^8.368*y)/g1^15 - (2*t^8.579*y)/g1^10 - (3*t^8.789*y)/g1^5 |
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 |
---|---|---|---|---|---|---|---|---|---|
1285 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}\tilde{q}_{1}^{2}$ | 0.7683 | 0.9711 | 0.7912 | [M:[0.8775, 1.0, 0.7551, 1.0, 0.8775, 0.7551, 0.6837], q:[0.5612, 0.5612], qb:[0.4388, 0.6837], phi:[0.4388]] | t^2.051 + 2*t^2.265 + 3*t^2.633 + 2*t^3. + t^4.102 + 4*t^4.316 + 3*t^4.53 + 7*t^4.684 + 6*t^4.898 + 4*t^5.051 + 9*t^5.265 + t^5.419 + 2*t^5.633 - 3*t^6. - t^4.316/y - t^4.316*y | detail |