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 |
---|---|---|---|---|---|---|---|---|---|
61104 | SU3adj1nf2 | ${}M_{1}\phi_{1}^{3}$ + ${ }q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}q_{2}^{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ | 1.2905 | 1.4467 | 0.892 | [X:[1.4], M:[1.1], q:[0.3, 0.7], qb:[0.7, 0.5], phi:[0.3]] | [X:[[0]], M:[[0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] | 0 | {a: 8259/6400, c: 9259/6400, X1: 7/5, M1: 11/10, q1: 3/10, q2: 7/10, qb1: 7/10, qb2: 1/2, phi1: 3/10} |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}q_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}^{3}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{2}^{2}$ | ${}q_{1}q_{2}\tilde{q}_{2}^{2}$ | 1 | t^2.4 + t^3. + 2*t^3.3 + t^3.6 + t^3.9 + 3*t^4.2 + t^4.5 + 2*t^4.8 + t^5.1 + 2*t^5.4 + 2*t^5.7 + t^6. + 2*t^6.3 + 6*t^6.6 + 2*t^6.9 + 6*t^7.2 + 5*t^7.5 + 7*t^7.8 + 6*t^8.1 + 6*t^8.4 + 6*t^8.7 + t^8.7/y^2 - t^3.9/y - t^4.8/y - t^6.3/y - t^6.9/y - (2*t^7.2)/y - t^7.5/y - t^7.8/y - (3*t^8.1)/y + t^8.7/y - t^3.9*y - t^4.8*y - t^6.3*y - t^6.9*y - 2*t^7.2*y - t^7.5*y - t^7.8*y - 3*t^8.1*y + t^8.7*y + t^8.7*y^2 | t^2.4 + t^3. + 2*t^3.3 + t^3.6 + t^3.9 + 3*t^4.2 + t^4.5 + 2*t^4.8 + t^5.1 + 2*t^5.4 + 2*t^5.7 + t^6. + 2*t^6.3 + 6*t^6.6 + 2*t^6.9 + 6*t^7.2 + 5*t^7.5 + 7*t^7.8 + 6*t^8.1 + 6*t^8.4 + 6*t^8.7 + t^8.7/y^2 - t^3.9/y - t^4.8/y - t^6.3/y - t^6.9/y - (2*t^7.2)/y - t^7.5/y - t^7.8/y - (3*t^8.1)/y + t^8.7/y - t^3.9*y - t^4.8*y - t^6.3*y - t^6.9*y - 2*t^7.2*y - t^7.5*y - t^7.8*y - 3*t^8.1*y + t^8.7*y + t^8.7*y^2 |
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 |
---|---|---|---|---|---|---|---|---|---|
58730 | SU3adj1nf2 | ${}M_{1}\phi_{1}^{3}$ + ${ }q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}q_{2}^{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | 1.412 | 1.5682 | 0.9004 | [X:[1.4], M:[1.1], q:[0.5, 0.6], qb:[0.5, 0.6], phi:[0.3]] | t^3. + 3*t^3.3 + t^3.6 + t^3.9 + 3*t^4.2 + t^4.5 + t^4.8 + 2*t^5.1 + t^5.4 - t^6. - t^3.9/y - t^4.8/y - t^3.9*y - t^4.8*y | detail | {a: 45183/32000, c: 50183/32000, X1: 7/5, M1: 11/10, q1: 1/2, q2: 3/5, qb1: 1/2, qb2: 3/5, phi1: 3/10} |