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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56616 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }M_{3}M_{5}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{1}X_{1}$ + ${ }M_{4}M_{6}$ + ${ }M_{7}q_{1}\tilde{q}_{2}$ | 0.7115 | 0.8814 | 0.8072 | [X:[1.2814], M:[0.7186, 0.6985, 0.99, 1.01, 1.01, 0.99, 0.7186], q:[0.7864, 0.495], qb:[0.5151, 0.495], phi:[0.4271]] | [X:[[6]], M:[[-6], [22], [14], [-14], [-14], [14], [-6]], q:[[-1], [7]], qb:[[-21], [7]], phi:[[2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{2}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{6}$, ${ }M_{4}$, ${ }M_{5}$, ${ }X_{1}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{7}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{7}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{5}$, ${ }M_{6}M_{7}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{4}M_{7}$, ${ }M_{5}M_{7}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$ | ${}M_{5}M_{6}$, ${ }M_{7}X_{1}$ | -2 | t^2.096 + t^2.156 + t^2.563 + t^2.97 + 2*t^3.03 + t^3.844 + t^4.191 + 4*t^4.251 + 3*t^4.312 + t^4.372 + t^4.658 + t^4.719 + t^5.065 + 4*t^5.126 + 2*t^5.186 + t^5.533 + 2*t^5.593 - 2*t^6. + t^6.06 + t^6.287 + 4*t^6.347 + 5*t^6.407 + 3*t^6.467 + t^6.528 + t^6.754 + 4*t^6.814 + 2*t^6.874 + t^6.935 + t^7.161 + 5*t^7.221 + 6*t^7.281 + 4*t^7.342 + 2*t^7.402 + t^7.628 + 2*t^7.688 - t^7.809 - t^8.096 - t^8.156 + t^8.382 + 4*t^8.442 + 9*t^8.503 + 4*t^8.563 + 6*t^8.623 + 3*t^8.683 + t^8.744 + t^8.849 + 4*t^8.91 - t^8.97 - t^4.281/y - t^6.377/y - t^6.437/y - t^6.844/y + t^7.251/y + t^7.658/y + (2*t^7.719)/y + t^8.065/y + (4*t^8.126)/y + (3*t^8.186)/y - t^8.472/y + t^8.593/y - t^4.281*y - t^6.377*y - t^6.437*y - t^6.844*y + t^7.251*y + t^7.658*y + 2*t^7.719*y + t^8.065*y + 4*t^8.126*y + 3*t^8.186*y - t^8.472*y + t^8.593*y | g1^22*t^2.096 + t^2.156/g1^6 + g1^4*t^2.563 + g1^14*t^2.97 + (2*t^3.03)/g1^14 + g1^6*t^3.844 + g1^44*t^4.191 + 4*g1^16*t^4.251 + (3*t^4.312)/g1^12 + t^4.372/g1^40 + g1^26*t^4.658 + t^4.719/g1^2 + g1^36*t^5.065 + 4*g1^8*t^5.126 + (2*t^5.186)/g1^20 + g1^18*t^5.533 + (2*t^5.593)/g1^10 - 2*t^6. + t^6.06/g1^28 + g1^66*t^6.287 + 4*g1^38*t^6.347 + 5*g1^10*t^6.407 + (3*t^6.467)/g1^18 + t^6.528/g1^46 + g1^48*t^6.754 + 4*g1^20*t^6.814 + (2*t^6.874)/g1^8 + t^6.935/g1^36 + g1^58*t^7.161 + 5*g1^30*t^7.221 + 6*g1^2*t^7.281 + (4*t^7.342)/g1^26 + (2*t^7.402)/g1^54 + g1^40*t^7.628 + 2*g1^12*t^7.688 - t^7.809/g1^44 - g1^22*t^8.096 - t^8.156/g1^6 + g1^88*t^8.382 + 4*g1^60*t^8.442 + 9*g1^32*t^8.503 + 4*g1^4*t^8.563 + (6*t^8.623)/g1^24 + (3*t^8.683)/g1^52 + t^8.744/g1^80 + g1^70*t^8.849 + 4*g1^42*t^8.91 - g1^14*t^8.97 - (g1^2*t^4.281)/y - (g1^24*t^6.377)/y - t^6.437/(g1^4*y) - (g1^6*t^6.844)/y + (g1^16*t^7.251)/y + (g1^26*t^7.658)/y + (2*t^7.719)/(g1^2*y) + (g1^36*t^8.065)/y + (4*g1^8*t^8.126)/y + (3*t^8.186)/(g1^20*y) - (g1^46*t^8.472)/y + t^8.593/(g1^10*y) - g1^2*t^4.281*y - g1^24*t^6.377*y - (t^6.437*y)/g1^4 - g1^6*t^6.844*y + g1^16*t^7.251*y + g1^26*t^7.658*y + (2*t^7.719*y)/g1^2 + g1^36*t^8.065*y + 4*g1^8*t^8.126*y + (3*t^8.186*y)/g1^20 - g1^46*t^8.472*y + (t^8.593*y)/g1^10 |
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 |
---|---|---|---|---|---|---|---|---|---|
54824 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }M_{3}M_{5}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{1}X_{1}$ + ${ }M_{4}M_{6}$ | 0.6914 | 0.8438 | 0.8194 | [X:[1.2806], M:[0.7194, 0.6954, 0.988, 1.012, 1.012, 0.988], q:[0.7866, 0.494], qb:[0.518, 0.494], phi:[0.4269]] | t^2.086 + t^2.561 + t^2.964 + 2*t^3.036 + 2*t^3.842 + t^4.172 + 3*t^4.245 + 2*t^4.317 + t^4.389 + t^4.647 + t^5.05 + 3*t^5.122 + t^5.525 + 2*t^5.597 + t^5.928 - 3*t^6. - t^4.281/y - t^4.281*y | detail |