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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60575 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }q_{2}^{2}\tilde{q}_{2}^{2}$ | 1.4059 | 1.6335 | 0.8606 | [X:[], M:[0.9286], q:[0.3286, 0.6143], qb:[0.5286, 0.3857], phi:[0.3571]] | [X:[], M:[[0]], q:[[-1], [-1]], qb:[[1], [1]], phi:[[0]]] | 1 | {a: 617229/439040, c: 717189/439040, M1: 13/14, q1: 23/70, q2: 43/70, qb1: 37/70, qb2: 27/70, phi1: 5/14} |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{5}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$ | ${}$ | -1 | 2*t^2.14 + t^2.57 + t^2.79 + t^3. + t^3.21 + t^3.43 + t^3.64 + t^4.07 + 4*t^4.29 + t^4.5 + 3*t^4.71 + t^4.89 + 2*t^4.93 + t^4.97 + 3*t^5.14 + 3*t^5.36 + t^5.4 + 4*t^5.57 + t^5.74 + 4*t^5.79 + t^5.96 - t^6. + t^6.04 + t^6.17 + 4*t^6.21 + 8*t^6.43 + t^6.47 + 4*t^6.64 + t^6.69 + t^6.81 + 8*t^6.86 - t^6.9 + 3*t^7.03 + 3*t^7.07 + 3*t^7.11 - t^7.24 + 9*t^7.29 + 7*t^7.5 + 3*t^7.54 + 10*t^7.71 + 3*t^7.89 + 9*t^7.93 + t^7.97 + 3*t^8.1 + 4*t^8.19 + 2*t^8.31 + 11*t^8.36 + 2*t^8.53 + 13*t^8.57 + 3*t^8.61 + t^8.74 + 8*t^8.79 + t^8.83 + 3*t^8.96 - t^4.07/y - t^5.14/y - (2*t^6.21)/y - t^6.64/y - t^6.86/y - t^7.07/y - t^7.29/y - t^7.5/y + t^7.71/y + (2*t^7.93)/y + t^8.14/y - t^8.36/y + (2*t^8.57)/y + t^8.79/y - t^4.07*y - t^5.14*y - 2*t^6.21*y - t^6.64*y - t^6.86*y - t^7.07*y - t^7.29*y - t^7.5*y + t^7.71*y + 2*t^7.93*y + t^8.14*y - t^8.36*y + 2*t^8.57*y + t^8.79*y | 2*t^2.14 + t^2.57 + t^2.79 + t^3. + t^3.21 + t^3.43 + t^3.64 + t^4.07 + 4*t^4.29 + t^4.5 + 3*t^4.71 + t^4.89/g1^3 + 2*t^4.93 + g1^3*t^4.97 + 3*t^5.14 + 3*t^5.36 + g1^3*t^5.4 + 4*t^5.57 + t^5.74/g1^3 + 4*t^5.79 + t^5.96/g1^3 - t^6. + g1^3*t^6.04 + t^6.17/g1^3 + 4*t^6.21 + 8*t^6.43 + g1^3*t^6.47 + 4*t^6.64 + g1^3*t^6.69 + t^6.81/g1^3 + 8*t^6.86 - g1^3*t^6.9 + (3*t^7.03)/g1^3 + 3*t^7.07 + 3*g1^3*t^7.11 - t^7.24/g1^3 + 9*t^7.29 + 7*t^7.5 + 3*g1^3*t^7.54 + 10*t^7.71 + (3*t^7.89)/g1^3 + 9*t^7.93 + g1^3*t^7.97 + (3*t^8.1)/g1^3 + 4*g1^3*t^8.19 + (2*t^8.31)/g1^3 + 11*t^8.36 + (2*t^8.53)/g1^3 + 13*t^8.57 + 3*g1^3*t^8.61 + t^8.74/g1^3 + 8*t^8.79 + g1^3*t^8.83 + (3*t^8.96)/g1^3 - t^4.07/y - t^5.14/y - (2*t^6.21)/y - t^6.64/y - t^6.86/y - t^7.07/y - t^7.29/y - t^7.5/y + t^7.71/y + (2*t^7.93)/y + t^8.14/y - t^8.36/y + (2*t^8.57)/y + t^8.79/y - t^4.07*y - t^5.14*y - 2*t^6.21*y - t^6.64*y - t^6.86*y - t^7.07*y - t^7.29*y - t^7.5*y + t^7.71*y + 2*t^7.93*y + t^8.14*y - t^8.36*y + 2*t^8.57*y + t^8.79*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 |
---|---|---|---|---|---|---|---|---|---|
57733 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{3}$ | 1.4299 | 1.6663 | 0.8581 | [X:[], M:[0.8964], q:[0.3877, 0.5019], qb:[0.5552, 0.348], phi:[0.3679]] | 2*t^2.21 + t^2.55 + t^2.69 + t^2.83 + t^3.17 + t^3.31 + t^3.65 + t^3.93 + t^4.27 + 4*t^4.41 + 3*t^4.76 + t^4.86 + 2*t^4.9 + t^4.94 + 3*t^5.04 + t^5.1 + t^5.24 + t^5.28 + 4*t^5.38 + t^5.48 + 3*t^5.52 + t^5.72 + 4*t^5.86 + t^5.96 - 2*t^6. - t^4.1/y - t^5.21/y - t^4.1*y - t^5.21*y | detail |