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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59658 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}^{5}$ + ${ }q_{2}\tilde{q}_{2}X_{1}$ + ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$ + ${ }M_{1}\phi_{1}^{3}$ | 1.3397 | 1.5772 | 0.8494 | [X:[1.4], M:[0.8], q:[0.5259, 0.337], qb:[0.4741, 0.263], phi:[0.4]] | [X:[[0]], M:[[0]], q:[[2], [-1]], qb:[[-2], [1]], phi:[[0]]] | 1 | {a: 4287/3200, c: 5047/3200, X1: 7/5, M1: 4/5, q1: 71/135, q2: 91/270, qb1: 64/135, qb2: 71/270, phi1: 2/5} |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }X_{1}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$ | ${3}\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{2}^{2}$ | 2 | t^2.37 + 2*t^2.4 + t^2.43 + 2*t^3. + t^3.57 + t^3.63 + 4*t^4.2 + t^4.73 + 3*t^4.77 + 5*t^4.8 + 4*t^4.83 + t^4.87 + 2*t^5.37 + 6*t^5.4 + t^5.43 + t^5.93 + 3*t^5.97 + 2*t^6. + 3*t^6.03 + t^6.07 + 5*t^6.57 + 8*t^6.6 + 4*t^6.63 + t^7.1 + 4*t^7.13 + 5*t^7.17 + 15*t^7.2 + 9*t^7.23 + 5*t^7.27 + t^7.3 + 2*t^7.73 + 10*t^7.77 + 8*t^7.8 + 7*t^7.83 + 2*t^7.87 + t^8.3 + 5*t^8.33 + 3*t^8.37 + 14*t^8.4 + 3*t^8.43 + 4*t^8.47 + t^8.5 + 4*t^8.93 + 14*t^8.97 - t^4.2/y - t^5.4/y - t^6.57/y - (2*t^6.6)/y - t^6.63/y - t^7.2/y + t^7.77/y + t^7.8/y + t^7.83/y + (2*t^8.37)/y + t^8.4/y + (2*t^8.43)/y - t^8.97/y - t^4.2*y - t^5.4*y - t^6.57*y - 2*t^6.6*y - t^6.63*y - t^7.2*y + t^7.77*y + t^7.8*y + t^7.83*y + 2*t^8.37*y + t^8.4*y + 2*t^8.43*y - t^8.97*y | g1^3*t^2.37 + 2*t^2.4 + t^2.43/g1^3 + 2*t^3. + g1^3*t^3.57 + t^3.63/g1^3 + 4*t^4.2 + g1^6*t^4.73 + 3*g1^3*t^4.77 + 5*t^4.8 + (4*t^4.83)/g1^3 + t^4.87/g1^6 + 2*g1^3*t^5.37 + 6*t^5.4 + t^5.43/g1^3 + g1^6*t^5.93 + 3*g1^3*t^5.97 + 2*t^6. + (3*t^6.03)/g1^3 + t^6.07/g1^6 + 5*g1^3*t^6.57 + 8*t^6.6 + (4*t^6.63)/g1^3 + g1^9*t^7.1 + 4*g1^6*t^7.13 + 5*g1^3*t^7.17 + 15*t^7.2 + (9*t^7.23)/g1^3 + (5*t^7.27)/g1^6 + t^7.3/g1^9 + 2*g1^6*t^7.73 + 10*g1^3*t^7.77 + 8*t^7.8 + (7*t^7.83)/g1^3 + (2*t^7.87)/g1^6 + g1^9*t^8.3 + 5*g1^6*t^8.33 + 3*g1^3*t^8.37 + 14*t^8.4 + (3*t^8.43)/g1^3 + (4*t^8.47)/g1^6 + t^8.5/g1^9 + 4*g1^6*t^8.93 + 14*g1^3*t^8.97 - t^4.2/y - t^5.4/y - (g1^3*t^6.57)/y - (2*t^6.6)/y - t^6.63/(g1^3*y) - t^7.2/y + (g1^3*t^7.77)/y + t^7.8/y + t^7.83/(g1^3*y) + (2*g1^3*t^8.37)/y + t^8.4/y + (2*t^8.43)/(g1^3*y) - (g1^3*t^8.97)/y - t^4.2*y - t^5.4*y - g1^3*t^6.57*y - 2*t^6.6*y - (t^6.63*y)/g1^3 - t^7.2*y + g1^3*t^7.77*y + t^7.8*y + (t^7.83*y)/g1^3 + 2*g1^3*t^8.37*y + t^8.4*y + (2*t^8.43*y)/g1^3 - g1^3*t^8.97*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 |
---|---|---|---|---|---|---|---|---|---|
57409 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}^{5}$ + ${ }q_{2}\tilde{q}_{2}X_{1}$ + ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$ | 1.3232 | 1.5482 | 0.8547 | [X:[1.4], q:[0.5259, 0.337], qb:[0.4741, 0.263], phi:[0.4]] | t^2.367 + t^2.4 + t^2.433 + 2*t^3. + t^3.567 + t^3.6 + t^3.633 + 4*t^4.2 + t^4.733 + 2*t^4.767 + 3*t^4.8 + 3*t^4.833 + t^4.867 + 2*t^5.367 + 4*t^5.4 + t^5.433 + t^5.933 + 3*t^5.967 + 3*t^6. - t^4.2/y - t^5.4/y - t^4.2*y - t^5.4*y | detail | {a: 21171/16000, c: 24771/16000, X1: 7/5, q1: 71/135, q2: 91/270, qb1: 64/135, qb2: 71/270, phi1: 2/5} |