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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58128 | SU3adj1nf2 | ${}M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{6}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ | 1.465 | 1.6733 | 0.8755 | [X:[1.3333], M:[0.9455, 0.7211], q:[0.5842, 0.4983], qb:[0.4703, 0.4472], phi:[0.3333]] | [X:[[0, 0]], M:[[-2, -1], [2, 1]], q:[[1, 1], [-2, -2]], qb:[[1, 0], [0, 1]], phi:[[0, 0]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{2}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ | ${}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$ | -1 | t^2.16 + 2*t^2.84 + t^2.91 + t^3. + t^3.09 + t^3.91 + t^4. + t^4.09 + t^4.16 + t^4.33 + t^4.84 + t^4.91 + 2*t^5. + t^5.07 + 2*t^5.09 + 3*t^5.16 + t^5.26 + 3*t^5.67 + 2*t^5.74 + t^5.81 + 2*t^5.84 + t^5.91 + t^5.93 - t^6. + 2*t^6.09 + 2*t^6.16 + t^6.19 + t^6.33 + t^6.49 + 2*t^6.74 + t^6.81 + 2*t^6.84 + 2*t^6.91 + t^6.93 + 3*t^7. + t^7.03 + t^7.07 + 3*t^7.09 + 4*t^7.16 + t^7.19 + 2*t^7.23 + t^7.26 + 3*t^7.33 + t^7.42 + t^7.48 + 2*t^7.67 + 3*t^7.74 + 2*t^7.81 + 2*t^7.84 + 2*t^7.91 + 3*t^7.93 + t^7.97 + 7*t^8. + 2*t^8.07 + 3*t^8.09 + t^8.16 + 2*t^8.19 + 3*t^8.26 + 2*t^8.33 + t^8.35 + t^8.49 + 4*t^8.51 + 2*t^8.58 + 2*t^8.65 + 3*t^8.67 + t^8.72 + 3*t^8.74 + t^8.77 + 2*t^8.81 - 4*t^8.84 - 2*t^8.91 + 3*t^8.93 - t^4./y - t^5./y - t^6.16/y - (2*t^6.84)/y - t^6.91/y - t^7./y - t^7.09/y - t^7.16/y - t^7.84/y - t^7.91/y + t^8./y + t^8.07/y - t^8.09/y + t^8.16/y + t^8.26/y - t^8.33/y + t^8.67/y + (2*t^8.74)/y + (2*t^8.84)/y + (2*t^8.93)/y - t^4.*y - t^5.*y - t^6.16*y - 2*t^6.84*y - t^6.91*y - t^7.*y - t^7.09*y - t^7.16*y - t^7.84*y - t^7.91*y + t^8.*y + t^8.07*y - t^8.09*y + t^8.16*y + t^8.26*y - t^8.33*y + t^8.67*y + 2*t^8.74*y + 2*t^8.84*y + 2*t^8.93*y | g1^2*g2*t^2.16 + (2*t^2.84)/(g1^2*g2) + t^2.91/(g1*g2^2) + t^3. + g1*g2^2*t^3.09 + t^3.91/(g1*g2^2) + t^4. + g1*g2^2*t^4.09 + g1^2*g2*t^4.16 + g1^4*g2^2*t^4.33 + t^4.84/(g1^2*g2) + t^4.91/(g1*g2^2) + 2*t^5. + (g1*t^5.07)/g2 + 2*g1*g2^2*t^5.09 + 3*g1^2*g2*t^5.16 + g1^3*g2^3*t^5.26 + (3*t^5.67)/(g1^4*g2^2) + (2*t^5.74)/(g1^3*g2^3) + t^5.81/(g1^2*g2^4) + (2*t^5.84)/(g1^2*g2) + t^5.91/(g1*g2^2) + (g2*t^5.93)/g1 - t^6. + 2*g1*g2^2*t^6.09 + 2*g1^2*g2*t^6.16 + g1^2*g2^4*t^6.19 + g1^4*g2^2*t^6.33 + g1^6*g2^3*t^6.49 + (2*t^6.74)/(g1^3*g2^3) + t^6.81/(g1^2*g2^4) + (2*t^6.84)/(g1^2*g2) + (2*t^6.91)/(g1*g2^2) + (g2*t^6.93)/g1 + 3*t^7. + g2^3*t^7.03 + (g1*t^7.07)/g2 + 3*g1*g2^2*t^7.09 + 4*g1^2*g2*t^7.16 + g1^2*g2^4*t^7.19 + 2*g1^3*t^7.23 + g1^3*g2^3*t^7.26 + 3*g1^4*g2^2*t^7.33 + g1^5*g2^4*t^7.42 + t^7.48/(g1^6*g2^6) + (2*t^7.67)/(g1^4*g2^2) + (3*t^7.74)/(g1^3*g2^3) + (2*t^7.81)/(g1^2*g2^4) + (2*t^7.84)/(g1^2*g2) + (2*t^7.91)/(g1*g2^2) + (3*g2*t^7.93)/g1 + t^7.97/g2^3 + 7*t^8. + (2*g1*t^8.07)/g2 + 3*g1*g2^2*t^8.09 + g1^2*g2*t^8.16 + 2*g1^2*g2^4*t^8.19 + 3*g1^3*g2^3*t^8.26 + 2*g1^4*g2^2*t^8.33 + g1^4*g2^5*t^8.35 + g1^6*g2^3*t^8.49 + (4*t^8.51)/(g1^6*g2^3) + (2*t^8.58)/(g1^5*g2^4) + t^8.65/(g1^4*g2^5) + g1^8*g2^4*t^8.65 + (3*t^8.67)/(g1^4*g2^2) + t^8.72/(g1^3*g2^6) + (3*t^8.74)/(g1^3*g2^3) + t^8.77/g1^3 + (2*t^8.81)/(g1^2*g2^4) - (4*t^8.84)/(g1^2*g2) - (2*t^8.91)/(g1*g2^2) + (3*g2*t^8.93)/g1 - t^4./y - t^5./y - (g1^2*g2*t^6.16)/y - (2*t^6.84)/(g1^2*g2*y) - t^6.91/(g1*g2^2*y) - t^7./y - (g1*g2^2*t^7.09)/y - (g1^2*g2*t^7.16)/y - t^7.84/(g1^2*g2*y) - t^7.91/(g1*g2^2*y) + t^8./y + (g1*t^8.07)/(g2*y) - (g1*g2^2*t^8.09)/y + (g1^2*g2*t^8.16)/y + (g1^3*g2^3*t^8.26)/y - (g1^4*g2^2*t^8.33)/y + t^8.67/(g1^4*g2^2*y) + (2*t^8.74)/(g1^3*g2^3*y) + (2*t^8.84)/(g1^2*g2*y) + (2*g2*t^8.93)/(g1*y) - t^4.*y - t^5.*y - g1^2*g2*t^6.16*y - (2*t^6.84*y)/(g1^2*g2) - (t^6.91*y)/(g1*g2^2) - t^7.*y - g1*g2^2*t^7.09*y - g1^2*g2*t^7.16*y - (t^7.84*y)/(g1^2*g2) - (t^7.91*y)/(g1*g2^2) + t^8.*y + (g1*t^8.07*y)/g2 - g1*g2^2*t^8.09*y + g1^2*g2*t^8.16*y + g1^3*g2^3*t^8.26*y - g1^4*g2^2*t^8.33*y + (t^8.67*y)/(g1^4*g2^2) + (2*t^8.74*y)/(g1^3*g2^3) + (2*t^8.84*y)/(g1^2*g2) + (2*g2*t^8.93*y)/g1 |
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 |
---|---|---|---|---|---|---|---|---|---|
57339 | SU3adj1nf2 | ${}M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{6}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$ | 1.4754 | 1.6837 | 0.8763 | [X:[1.3333], M:[0.9697, 0.697], q:[0.5152, 0.4848], qb:[0.5152, 0.4848], phi:[0.3333]] | t^2.091 + 2*t^2.909 + 3*t^3. + 3*t^4. + t^4.091 + t^4.182 + t^4.909 + 4*t^5. + 4*t^5.091 + 2*t^5.455 + 2*t^5.545 + 3*t^5.818 + 4*t^5.909 + 2*t^6. - t^4./y - t^5./y - t^4.*y - t^5.*y | detail | {a: 779/528, c: 889/528, X1: 4/3, M1: 32/33, M2: 23/33, q1: 17/33, q2: 16/33, qb1: 17/33, qb2: 16/33, phi1: 1/3} |