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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58778 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{1}$ + ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$ + ${ }M_{1}\phi_{1}^{2}q_{2}\tilde{q}_{2}$ | 1.2394 | 1.4544 | 0.8522 | [X:[1.4406], M:[0.7203], q:[0.7995, 0.2401], qb:[0.4802, 0.3193], phi:[0.3601]] | [X:[[6]], M:[[3]], q:[[-5], [1]], qb:[[2], [-7]], phi:[[1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}\phi_{1}^{2}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{5}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{2}^{3}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$ | ${}M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{4}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | 3 | 3*t^2.16 + t^2.76 + 2*t^3.24 + t^3.36 + t^3.84 + 7*t^4.32 + 2*t^4.44 + 6*t^4.92 + 6*t^5.4 + 5*t^5.52 + 3*t^6. + 2*t^6.12 + 14*t^6.48 + 8*t^6.6 + t^6.71 + 13*t^7.08 + 3*t^7.2 + 12*t^7.56 + 14*t^7.68 + 2*t^7.79 + 7*t^8.16 + 9*t^8.28 + 24*t^8.64 + 13*t^8.76 + 8*t^8.87 - t^4.08/y - t^5.16/y - (3*t^6.24)/y - t^7.32/y - t^7.44/y + (3*t^7.92)/y - (2*t^8.4)/y + (2*t^8.52)/y - t^4.08*y - t^5.16*y - 3*t^6.24*y - t^7.32*y - t^7.44*y + 3*t^7.92*y - 2*t^8.4*y + 2*t^8.52*y | g1^2*t^2.16 + 2*g1^3*t^2.16 + t^2.76/g1^5 + g1^3*t^3.24 + g1^4*t^3.24 + t^3.36/g1^12 + t^3.84/g1^4 + g1^4*t^4.32 + 3*g1^5*t^4.32 + 3*g1^6*t^4.32 + (2*t^4.44)/g1^11 + t^4.92/g1^3 + (5*t^4.92)/g1^2 + g1^5*t^5.4 + 4*g1^6*t^5.4 + g1^7*t^5.4 + (4*t^5.52)/g1^10 + t^5.52/g1^9 - 5*t^6. + (2*t^6.)/g1^2 + (6*t^6.)/g1 + t^6.12/g1^18 + t^6.12/g1^17 + 2*g1^6*t^6.48 + 4*g1^7*t^6.48 + 5*g1^8*t^6.48 + 3*g1^9*t^6.48 + (5*t^6.6)/g1^9 + (4*t^6.6)/g1^8 - t^6.6/g1^7 + t^6.71/g1^24 + 9*t^7.08 + (2*t^7.08)/g1 + 3*g1*t^7.08 - g1^2*t^7.08 + (3*t^7.2)/g1^16 + g1^7*t^7.56 + 5*g1^8*t^7.56 + 8*g1^9*t^7.56 - 2*g1^10*t^7.56 + (7*t^7.68)/g1^8 + (10*t^7.68)/g1^7 - (3*t^7.68)/g1^6 + (2*t^7.79)/g1^23 + 2*t^8.16 + 13*g1*t^8.16 + 3*g1^2*t^8.16 - 11*g1^3*t^8.16 + t^8.28/g1^16 + (7*t^8.28)/g1^15 + (3*t^8.28)/g1^14 - (2*t^8.28)/g1^13 + 2*g1^8*t^8.64 + 7*g1^9*t^8.64 + 8*g1^10*t^8.64 + 2*g1^11*t^8.64 + 5*g1^12*t^8.64 + (8*t^8.76)/g1^7 + (17*t^8.76)/g1^6 - (7*t^8.76)/g1^5 - (5*t^8.76)/g1^4 + t^8.87/g1^23 + (7*t^8.87)/g1^22 - (g1*t^4.08)/y - (g1^2*t^5.16)/y - (g1^3*t^6.24)/y - (2*g1^4*t^6.24)/y - (2*g1^4*t^7.32)/y + (g1^6*t^7.32)/y - t^7.44/(g1^11*y) + (2*t^7.92)/(g1^2*y) + t^7.92/(g1*y) - (g1^5*t^8.4)/y - (g1^7*t^8.4)/y + (2*t^8.52)/(g1^9*y) - g1*t^4.08*y - g1^2*t^5.16*y - g1^3*t^6.24*y - 2*g1^4*t^6.24*y - 2*g1^4*t^7.32*y + g1^6*t^7.32*y - (t^7.44*y)/g1^11 + (2*t^7.92*y)/g1^2 + (t^7.92*y)/g1 - g1^5*t^8.4*y - g1^7*t^8.4*y + (2*t^8.52*y)/g1^9 |
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 |
---|---|---|---|---|---|---|---|---|---|
57756 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{1}$ + ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$ | 1.2193 | 1.4171 | 0.8604 | [X:[1.4431], M:[], q:[0.7975, 0.2405], qb:[0.481, 0.3164], phi:[0.3608]] | 2*t^2.16 + t^2.75 + 2*t^3.25 + t^3.34 + 2*t^3.84 + 4*t^4.33 + 2*t^4.42 + 5*t^4.92 + 4*t^5.41 + 4*t^5.51 + 4*t^6. - t^4.08/y - t^5.16/y - t^4.08*y - t^5.16*y | detail |