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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58822 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{1}$ | 1.351 | 1.5433 | 0.8754 | [X:[1.3845], M:[0.9233, 0.6922], q:[0.6411, 0.41], qb:[0.3589, 0.7434], phi:[0.3078]] | [X:[[0, 2]], M:[[0, -3], [0, 1]], q:[[-1, 2], [-1, 6]], qb:[[1, -2], [1, 0]], phi:[[0, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{1}$, ${ }\phi_{1}^{3}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}\phi_{1}^{3}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{6}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ | ${}\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{3}$ | 0 | t^2.08 + t^2.31 + 2*t^2.77 + t^3. + t^3.46 + 4*t^4.15 + 2*t^4.38 + t^4.61 + 2*t^4.85 + 4*t^5.08 + 3*t^5.31 + 4*t^5.54 + 2*t^5.77 + 7*t^6.23 + 8*t^6.46 + 7*t^6.92 + 7*t^7.15 + 6*t^7.38 + 7*t^7.61 + 2*t^7.62 + 2*t^7.84 + 3*t^7.85 + t^8.07 + 15*t^8.31 + 15*t^8.54 + 8*t^8.77 + t^8.77/y^2 - t^3.92/y - t^4.85/y - t^6./y - t^6.23/y - (2*t^6.69)/y - (2*t^6.92)/y - (2*t^7.62)/y + (2*t^7.85)/y + t^8.08/y - t^8.31/y + t^8.54/y + (2*t^8.77)/y - t^3.92*y - t^4.85*y - t^6.*y - t^6.23*y - 2*t^6.69*y - 2*t^6.92*y - 2*t^7.62*y + 2*t^7.85*y + t^8.08*y - t^8.31*y + t^8.54*y + 2*t^8.77*y + t^8.77*y^2 | g2*t^2.08 + g2^4*t^2.31 + (2*t^2.77)/g2^3 + t^3. + g2^6*t^3.46 + 4*g2^2*t^4.15 + 2*g2^5*t^4.38 + g2^8*t^4.61 + (2*t^4.85)/g2^2 + 4*g2*t^5.08 + (g1^3*t^5.31)/g2^5 + g2^4*t^5.31 + (g2^13*t^5.31)/g1^3 + (3*t^5.54)/g2^6 + g2^7*t^5.54 + t^5.77/g2^3 + g2^10*t^5.77 - 2*t^6. + (g1^3*t^6.)/g2^9 + (g2^9*t^6.)/g1^3 + (g1^3*t^6.23)/g2^6 + 5*g2^3*t^6.23 + (g2^12*t^6.23)/g1^3 + (g1^3*t^6.46)/g2^3 + 6*g2^6*t^6.46 + (g2^15*t^6.46)/g1^3 - (2*t^6.69)/g2^4 + 2*g2^9*t^6.69 + (5*t^6.92)/g2 + 2*g2^12*t^6.92 + 7*g2^2*t^7.15 + (g1^3*t^7.38)/g2^4 + 4*g2^5*t^7.38 + (g2^14*t^7.38)/g1^3 + (g1^3*t^7.61)/g2 + 5*g2^8*t^7.61 + (g2^17*t^7.61)/g1^3 + (2*t^7.62)/g2^5 + 2*g2^11*t^7.84 - (g1^3*t^7.85)/g2^11 + (5*t^7.85)/g2^2 - (g2^7*t^7.85)/g1^3 + g2^14*t^8.07 + (g1^3*t^8.08)/g2^8 - 2*g2*t^8.08 + (g2^10*t^8.08)/g1^3 + (4*t^8.31)/g2^9 + (2*g1^3*t^8.31)/g2^5 + 7*g2^4*t^8.31 + (2*g2^13*t^8.31)/g1^3 + t^8.54/g2^6 + (2*g1^3*t^8.54)/g2^2 + 10*g2^7*t^8.54 + (2*g2^16*t^8.54)/g1^3 + (g1^3*t^8.77)/g2^12 - (5*t^8.77)/g2^3 + 2*g1^3*g2*t^8.77 + (g2^6*t^8.77)/g1^3 + 7*g2^10*t^8.77 + (2*g2^19*t^8.77)/g1^3 + t^8.77/(g2^3*y^2) - t^3.92/(g2*y) - t^4.85/(g2^2*y) - t^6./y - (g2^3*t^6.23)/y - (2*t^6.69)/(g2^4*y) - (2*t^6.92)/(g2*y) - (2*t^7.62)/(g2^5*y) + (2*t^7.85)/(g2^2*y) + (g2*t^8.08)/y - (g2^4*t^8.31)/y + t^8.54/(g2^6*y) + t^8.77/(g2^3*y) + (g2^10*t^8.77)/y - (t^3.92*y)/g2 - (t^4.85*y)/g2^2 - t^6.*y - g2^3*t^6.23*y - (2*t^6.69*y)/g2^4 - (2*t^6.92*y)/g2 - (2*t^7.62*y)/g2^5 + (2*t^7.85*y)/g2^2 + g2*t^8.08*y - g2^4*t^8.31*y + (t^8.54*y)/g2^6 + (t^8.77*y)/g2^3 + g2^10*t^8.77*y + (t^8.77*y^2)/g2^3 |
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 |
---|---|---|---|---|---|---|---|---|---|
57412 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ | 1.3303 | 1.5033 | 0.8849 | [X:[1.385], M:[0.9225], q:[0.6408, 0.4108], qb:[0.3592, 0.7442], phi:[0.3075]] | t^2.31 + 2*t^2.767 + t^3. + t^3.465 + t^3.922 + 3*t^4.155 + t^4.388 + t^4.62 + 3*t^5.078 + 3*t^5.31 + 3*t^5.535 + t^5.767 + t^5.775 - t^3.922/y - t^4.845/y - t^3.922*y - t^4.845*y | detail |