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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6698 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}M_{6}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ + ${ }M_{8}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{8}^{2}$ | 0.6042 | 0.7878 | 0.767 | [M:[0.9375, 0.8125, 1.0625, 0.6875, 1.3125, 0.6875, 0.75, 1.0], q:[0.6563, 0.4063], qb:[0.2813, 0.9063], phi:[0.4375]] | [M:[[0], [0], [0], [0], [0], [0], [0], [0]], q:[[0], [0]], qb:[[0], [0]], phi:[[0]]] | 0 | {a: 79197/131072, c: 103261/131072, M1: 15/16, M2: 13/16, M3: 17/16, M4: 11/16, M5: 21/16, M6: 11/16, M7: 3/4, M8: 1, q1: 21/32, q2: 13/32, qb1: 9/32, qb2: 29/32, phi1: 7/16} |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{4}$, ${ }M_{6}$, ${ }M_{7}$, ${ }M_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{8}$, ${ }M_{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{6}$, ${ }M_{7}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{2}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{6}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{7}$, ${ }M_{4}M_{8}$, ${ }M_{6}M_{8}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{6}$, ${ }M_{7}M_{8}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}M_{7}$, ${ }M_{2}M_{8}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{8}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{8}$, ${ }M_{3}\phi_{1}^{2}$ | ${}\phi_{1}^{3}q_{2}\tilde{q}_{1}$ | 0 | 2*t^2.063 + t^2.25 + t^2.438 + t^2.625 + t^2.813 + t^3. + t^3.188 + t^3.375 + 3*t^4.125 + 2*t^4.313 + 3*t^4.5 + 4*t^4.688 + 4*t^4.875 + 4*t^5.063 + 5*t^5.25 + 4*t^5.438 + 3*t^5.625 + 2*t^5.813 + 4*t^6.188 + 3*t^6.375 + 4*t^6.563 + 5*t^6.75 + 7*t^6.938 + 8*t^7.125 + 10*t^7.313 + 10*t^7.5 + 9*t^7.688 + 8*t^7.875 + 3*t^8.063 + 6*t^8.25 + 3*t^8.438 + 3*t^8.625 + 3*t^8.813 - t^4.313/y - t^6.375/y - t^6.563/y - t^6.75/y - t^6.938/y + t^7.125/y + (2*t^7.313)/y + (2*t^7.5)/y + (4*t^7.688)/y + (4*t^7.875)/y + (5*t^8.063)/y + (5*t^8.25)/y + (4*t^8.438)/y + (2*t^8.625)/y + t^8.813/y - t^4.313*y - t^6.375*y - t^6.563*y - t^6.75*y - t^6.938*y + t^7.125*y + 2*t^7.313*y + 2*t^7.5*y + 4*t^7.688*y + 4*t^7.875*y + 5*t^8.063*y + 5*t^8.25*y + 4*t^8.438*y + 2*t^8.625*y + t^8.813*y | 2*t^2.063 + t^2.25 + t^2.438 + t^2.625 + t^2.813 + t^3. + t^3.188 + t^3.375 + 3*t^4.125 + 2*t^4.313 + 3*t^4.5 + 4*t^4.688 + 4*t^4.875 + 4*t^5.063 + 5*t^5.25 + 4*t^5.438 + 3*t^5.625 + 2*t^5.813 + 4*t^6.188 + 3*t^6.375 + 4*t^6.563 + 5*t^6.75 + 7*t^6.938 + 8*t^7.125 + 10*t^7.313 + 10*t^7.5 + 9*t^7.688 + 8*t^7.875 + 3*t^8.063 + 6*t^8.25 + 3*t^8.438 + 3*t^8.625 + 3*t^8.813 - t^4.313/y - t^6.375/y - t^6.563/y - t^6.75/y - t^6.938/y + t^7.125/y + (2*t^7.313)/y + (2*t^7.5)/y + (4*t^7.688)/y + (4*t^7.875)/y + (5*t^8.063)/y + (5*t^8.25)/y + (4*t^8.438)/y + (2*t^8.625)/y + t^8.813/y - t^4.313*y - t^6.375*y - t^6.563*y - t^6.75*y - t^6.938*y + t^7.125*y + 2*t^7.313*y + 2*t^7.5*y + 4*t^7.688*y + 4*t^7.875*y + 5*t^8.063*y + 5*t^8.25*y + 4*t^8.438*y + 2*t^8.625*y + t^8.813*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 |
---|---|---|---|---|---|---|---|---|---|
5095 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}M_{6}$ + ${ }\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ + ${ }M_{8}\phi_{1}\tilde{q}_{1}^{2}$ | 0.6294 | 0.818 | 0.7694 | [M:[1.0178, 0.6864, 0.9822, 0.7219, 1.2781, 0.7219, 0.8876, 0.8166], q:[0.6391, 0.3432], qb:[0.3787, 0.9349], phi:[0.426]] | t^2.059 + 2*t^2.166 + t^2.45 + t^2.556 + t^2.663 + t^2.947 + t^3.053 + t^3.444 + t^4.118 + 2*t^4.225 + 3*t^4.331 + t^4.509 + 3*t^4.615 + 4*t^4.722 + 2*t^4.828 + t^4.899 + 2*t^5.006 + 5*t^5.112 + 3*t^5.219 + t^5.325 + t^5.396 + 2*t^5.503 + 3*t^5.609 + t^5.716 + t^5.893 - t^6. - t^4.278/y - t^4.278*y | detail |