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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60956 | SU3adj1nf2 | ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | 1.3352 | 1.6107 | 0.829 | [X:[], M:[0.8, 0.7923], q:[0.5333, 0.5333], qb:[0.2744, 0.2589], phi:[0.4]] | [X:[], M:[[0], [1]], q:[[0], [0]], qb:[[-1], [1]], phi:[[0]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$, ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{2}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}\tilde{q}_{2}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}^{3}$, ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${}M_{2}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ 3}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$ | 6 | 3*t^2.38 + 2*t^2.4 + 2*t^2.42 + 3*t^3.58 + 2*t^3.62 + 6*t^4.75 + 9*t^4.78 + 9*t^4.8 + 7*t^4.82 + 3*t^4.85 + t^5.93 + 8*t^5.95 + 7*t^5.98 + 6*t^6. + 5*t^6.02 + 3*t^6.05 + t^6.07 + 10*t^7.13 + 24*t^7.15 + 24*t^7.18 + 27*t^7.2 + 18*t^7.22 + 12*t^7.25 + 4*t^7.27 + 3*t^8.31 + 16*t^8.33 + 25*t^8.35 + 16*t^8.38 + 23*t^8.4 + 9*t^8.42 + 12*t^8.45 + 5*t^8.47 + 2*t^8.49 - t^4.2/y - t^5.4/y - (3*t^6.58)/y - (2*t^6.6)/y - (2*t^6.62)/y + (3*t^7.75)/y + (3*t^7.78)/y + (6*t^7.8)/y + (3*t^7.82)/y + t^7.85/y + (3*t^8.95)/y - (2*t^8.98)/y - t^4.2*y - t^5.4*y - 3*t^6.58*y - 2*t^6.6*y - 2*t^6.62*y + 3*t^7.75*y + 3*t^7.78*y + 6*t^7.8*y + 3*t^7.82*y + t^7.85*y + 3*t^8.95*y - 2*t^8.98*y | 3*g1*t^2.38 + 2*t^2.4 + (2*t^2.42)/g1 + 3*g1*t^3.58 + (2*t^3.62)/g1 + 6*g1^2*t^4.75 + 9*g1*t^4.78 + 9*t^4.8 + (7*t^4.82)/g1 + (3*t^4.85)/g1^2 + g1^3*t^5.93 + 8*g1^2*t^5.95 + 7*g1*t^5.98 + 6*t^6. + (5*t^6.02)/g1 + (3*t^6.05)/g1^2 + t^6.07/g1^3 + 10*g1^3*t^7.13 + 24*g1^2*t^7.15 + 24*g1*t^7.18 + 27*t^7.2 + (18*t^7.22)/g1 + (12*t^7.25)/g1^2 + (4*t^7.27)/g1^3 + 3*g1^4*t^8.31 + 16*g1^3*t^8.33 + 25*g1^2*t^8.35 + 16*g1*t^8.38 + 23*t^8.4 + (9*t^8.42)/g1 + (12*t^8.45)/g1^2 + (5*t^8.47)/g1^3 + (2*t^8.49)/g1^4 - t^4.2/y - t^5.4/y - (3*g1*t^6.58)/y - (2*t^6.6)/y - (2*t^6.62)/(g1*y) + (3*g1^2*t^7.75)/y + (3*g1*t^7.78)/y + (6*t^7.8)/y + (3*t^7.82)/(g1*y) + t^7.85/(g1^2*y) + (3*g1^2*t^8.95)/y - (2*g1*t^8.98)/y - t^4.2*y - t^5.4*y - 3*g1*t^6.58*y - 2*t^6.6*y - (2*t^6.62*y)/g1 + 3*g1^2*t^7.75*y + 3*g1*t^7.78*y + 6*t^7.8*y + (3*t^7.82*y)/g1 + (t^7.85*y)/g1^2 + 3*g1^2*t^8.95*y - 2*g1*t^8.98*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 |
---|---|---|---|---|---|---|---|---|---|
59492 | SU3adj1nf2 | ${}\phi_{1}^{5}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ | 1.3185 | 1.581 | 0.834 | [X:[], M:[0.8], q:[0.5333, 0.5333], qb:[0.2667, 0.2667], phi:[0.4]] | 6*t^2.4 + 6*t^3.6 + 27*t^4.8 + 32*t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y | detail | {a: 2637/2000, c: 1581/1000, M1: 4/5, q1: 8/15, q2: 8/15, qb1: 4/15, qb2: 4/15, phi1: 2/5} |