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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56335 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}X_{1}$ + ${ }M_{3}\phi_{1}q_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{1}q_{2}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{1}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{7}$ | 0.6633 | 0.8388 | 0.7907 | [X:[1.6], M:[1.2, 0.4, 0.7831, 0.8, 0.8169, 0.7915, 0.8], q:[0.4085, 0.3915], qb:[0.8, 0.8], phi:[0.4]] | [X:[[0]], M:[[0], [0], [2], [0], [-2], [1], [0]], q:[[-1], [1]], qb:[[0], [0]], phi:[[0]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{3}$, ${ }M_{6}$, ${ }M_{4}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{3}M_{4}$, ${ }M_{6}^{2}$, ${ }M_{3}M_{7}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }X_{1}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}M_{7}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{5}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }M_{6}q_{2}\tilde{q}_{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{7}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{7}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$ | ${}\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$ | -2 | t^2.349 + t^2.375 + 3*t^2.4 + t^2.451 + 2*t^3.575 + t^3.625 + t^4.699 + t^4.724 + 4*t^4.749 + 3*t^4.775 + 8*t^4.8 + t^4.825 + 3*t^4.851 + t^4.901 + 2*t^5.924 + t^5.949 + 5*t^5.975 - 2*t^6. + 3*t^6.025 - t^6.051 + t^6.076 + t^7.048 + t^7.073 + 4*t^7.099 + 4*t^7.124 + 12*t^7.149 + 4*t^7.175 + 14*t^7.2 - t^7.225 + 7*t^7.251 + t^7.276 + 3*t^7.301 + t^7.352 + 2*t^8.273 + t^8.299 + 6*t^8.324 - 2*t^8.349 + 7*t^8.375 - 9*t^8.4 + 3*t^8.425 - 6*t^8.451 + 3*t^8.476 - t^8.501 + t^8.527 - t^4.2/y - t^6.549/y - t^6.575/y - (2*t^6.6)/y - t^6.651/y + t^7.724/y + (4*t^7.749)/y + (3*t^7.775)/y + (6*t^7.8)/y + (2*t^7.825)/y + (4*t^7.851)/y - t^8.899/y + t^8.924/y - t^8.949/y + (5*t^8.975)/y - t^4.2*y - t^6.549*y - t^6.575*y - 2*t^6.6*y - t^6.651*y + t^7.724*y + 4*t^7.749*y + 3*t^7.775*y + 6*t^7.8*y + 2*t^7.825*y + 4*t^7.851*y - t^8.899*y + t^8.924*y - t^8.949*y + 5*t^8.975*y | g1^2*t^2.349 + g1*t^2.375 + 3*t^2.4 + t^2.451/g1^2 + 2*g1*t^3.575 + t^3.625/g1 + g1^4*t^4.699 + g1^3*t^4.724 + 4*g1^2*t^4.749 + 3*g1*t^4.775 + 8*t^4.8 + t^4.825/g1 + (3*t^4.851)/g1^2 + t^4.901/g1^4 + 2*g1^3*t^5.924 + g1^2*t^5.949 + 5*g1*t^5.975 - 2*t^6. + (3*t^6.025)/g1 - t^6.051/g1^2 + t^6.076/g1^3 + g1^6*t^7.048 + g1^5*t^7.073 + 4*g1^4*t^7.099 + 4*g1^3*t^7.124 + 12*g1^2*t^7.149 + 4*g1*t^7.175 + 14*t^7.2 - t^7.225/g1 + (7*t^7.251)/g1^2 + t^7.276/g1^3 + (3*t^7.301)/g1^4 + t^7.352/g1^6 + 2*g1^5*t^8.273 + g1^4*t^8.299 + 6*g1^3*t^8.324 - 2*g1^2*t^8.349 + 7*g1*t^8.375 - 9*t^8.4 + (3*t^8.425)/g1 - (6*t^8.451)/g1^2 + (3*t^8.476)/g1^3 - t^8.501/g1^4 + t^8.527/g1^5 - t^4.2/y - (g1^2*t^6.549)/y - (g1*t^6.575)/y - (2*t^6.6)/y - t^6.651/(g1^2*y) + (g1^3*t^7.724)/y + (4*g1^2*t^7.749)/y + (3*g1*t^7.775)/y + (6*t^7.8)/y + (2*t^7.825)/(g1*y) + (4*t^7.851)/(g1^2*y) - (g1^4*t^8.899)/y + (g1^3*t^8.924)/y - (g1^2*t^8.949)/y + (5*g1*t^8.975)/y - t^4.2*y - g1^2*t^6.549*y - g1*t^6.575*y - 2*t^6.6*y - (t^6.651*y)/g1^2 + g1^3*t^7.724*y + 4*g1^2*t^7.749*y + 3*g1*t^7.775*y + 6*t^7.8*y + (2*t^7.825*y)/g1 + (4*t^7.851*y)/g1^2 - g1^4*t^8.899*y + g1^3*t^8.924*y - g1^2*t^8.949*y + 5*g1*t^8.975*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 |
---|---|---|---|---|---|---|---|---|---|
52231 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}X_{1}$ + ${ }M_{3}\phi_{1}q_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{1}q_{2}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{1}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ | 0.6468 | 0.8098 | 0.7987 | [X:[1.6], M:[1.2, 0.4, 0.7831, 0.8, 0.8169, 0.7915], q:[0.4085, 0.3915], qb:[0.8, 0.8], phi:[0.4]] | t^2.349 + t^2.375 + 2*t^2.4 + t^2.451 + 2*t^3.575 + t^3.6 + t^3.625 + t^4.699 + t^4.724 + 3*t^4.749 + 2*t^4.775 + 5*t^4.8 + t^4.825 + 2*t^4.851 + t^4.901 + 2*t^5.924 + 2*t^5.949 + 4*t^5.975 - t^4.2/y - t^4.2*y | detail |