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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59456 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$ | 1.4745 | 1.6845 | 0.8753 | [X:[1.328], M:[0.992, 0.68], q:[0.492, 0.4999], qb:[0.508, 0.4841], phi:[0.336]] | [X:[[0, 2]], M:[[0, 3], [0, -5]], q:[[-1, 9], [-1, 6]], qb:[[1, -9], [1, 0]], phi:[[0, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{2}\phi_{1}^{3}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$ | ${}$ | -2 | t^2.04 + t^2.93 + t^2.95 + t^2.98 + t^3. + t^3.02 + t^3.94 + t^3.98 + t^4.01 + t^4.03 + t^4.08 + t^4.94 + 2*t^4.97 + t^4.99 + 2*t^5.02 + 2*t^5.04 + t^5.06 + t^5.44 + t^5.46 + t^5.48 + t^5.51 + t^5.86 + t^5.88 + 2*t^5.9 + t^5.93 + 3*t^5.95 + 2*t^5.98 - 2*t^6. + t^6.02 + 2*t^6.05 + t^6.12 + t^6.44 + t^6.47 + t^6.49 + t^6.52 + t^6.86 + t^6.89 + 2*t^6.91 + 2*t^6.94 + 4*t^6.96 + 3*t^6.98 + 2*t^7.01 + 2*t^7.03 + 3*t^7.06 + t^7.08 + t^7.1 + t^7.38 + t^7.45 + t^7.48 + t^7.5 + 2*t^7.52 + t^7.55 + t^7.6 + 2*t^7.87 + 3*t^7.9 + 3*t^7.92 + 4*t^7.94 + 6*t^7.97 + 5*t^7.99 + 3*t^8.02 + 3*t^8.06 + t^8.09 + t^8.16 + t^8.37 + 2*t^8.39 + 2*t^8.41 + 2*t^8.44 + 2*t^8.46 + t^8.48 - t^8.56 - t^8.58 + t^8.78 + t^8.81 + 2*t^8.83 + 2*t^8.86 + 4*t^8.88 + 4*t^8.9 + t^8.95 + 3*t^8.98 - t^4.01/y - t^5.02/y - t^6.05/y - t^6.94/y - t^6.96/y - t^6.98/y - t^7.01/y - t^7.03/y - t^7.06/y - t^7.94/y + t^7.97/y + t^8.06/y - t^8.09/y + t^8.88/y + t^8.9/y + (2*t^8.93)/y + t^8.95/y + (2*t^8.98)/y - t^4.01*y - t^5.02*y - t^6.05*y - t^6.94*y - t^6.96*y - t^6.98*y - t^7.01*y - t^7.03*y - t^7.06*y - t^7.94*y + t^7.97*y + t^8.06*y - t^8.09*y + t^8.88*y + t^8.9*y + 2*t^8.93*y + t^8.95*y + 2*t^8.98*y | t^2.04/g2^5 + g2^9*t^2.93 + g2^6*t^2.95 + g2^3*t^2.98 + t^3. + t^3.02/g2^3 + g2^8*t^3.94 + g2^2*t^3.98 + t^4.01/g2 + t^4.03/g2^4 + t^4.08/g2^10 + g2^7*t^4.94 + 2*g2^4*t^4.97 + g2*t^4.99 + (2*t^5.02)/g2^2 + (2*t^5.04)/g2^5 + t^5.06/g2^8 + (g1^3*t^5.44)/g2^10 + (g2^23*t^5.46)/g1^3 + (g2^20*t^5.48)/g1^3 + (g1^3*t^5.51)/g2^19 + g2^18*t^5.86 + g2^15*t^5.88 + 2*g2^12*t^5.9 + g2^9*t^5.93 + 3*g2^6*t^5.95 + 2*g2^3*t^5.98 - 2*t^6. + t^6.02/g2^3 + (2*t^6.05)/g2^6 + t^6.12/g2^15 + (g1^3*t^6.44)/g2^11 + (g2^22*t^6.47)/g1^3 + (g2^19*t^6.49)/g1^3 + (g1^3*t^6.52)/g2^20 + g2^17*t^6.86 + g2^14*t^6.89 + 2*g2^11*t^6.91 + 2*g2^8*t^6.94 + 4*g2^5*t^6.96 + 3*g2^2*t^6.98 + (2*t^7.01)/g2 + (2*t^7.03)/g2^4 + (3*t^7.06)/g2^7 + t^7.08/g2^10 + t^7.1/g2^13 + (g1^3*t^7.38)/g2^3 + (g1^3*t^7.45)/g2^12 + (g2^21*t^7.48)/g1^3 - (g1^3*t^7.5)/g2^18 + (2*g2^18*t^7.5)/g1^3 + (g1^3*t^7.52)/g2^21 + (g2^15*t^7.52)/g1^3 + (g1^3*t^7.55)/g2^24 + (g1^3*t^7.6)/g2^30 + 2*g2^16*t^7.87 + 3*g2^13*t^7.9 + 3*g2^10*t^7.92 + 4*g2^7*t^7.94 + 6*g2^4*t^7.97 + 5*g2*t^7.99 + (3*t^8.02)/g2^2 + (3*t^8.06)/g2^8 + t^8.09/g2^11 + t^8.16/g2^20 + (g1^3*t^8.37)/g2 + (g1^3*t^8.39)/g2^4 + (g2^32*t^8.39)/g1^3 + (2*g2^29*t^8.41)/g1^3 + (g1^3*t^8.44)/g2^10 + (g2^26*t^8.44)/g1^3 + (2*g1^3*t^8.46)/g2^13 + (g2^20*t^8.48)/g1^3 - (g1^3*t^8.51)/g2^19 + (g2^17*t^8.51)/g1^3 + (g1^3*t^8.53)/g2^22 - (g2^14*t^8.53)/g1^3 - (g2^11*t^8.56)/g1^3 - (g1^3*t^8.58)/g2^28 + g2^27*t^8.78 + g2^24*t^8.81 + 2*g2^21*t^8.83 + 2*g2^18*t^8.86 + 4*g2^15*t^8.88 + 4*g2^12*t^8.9 + g2^6*t^8.95 + 3*g2^3*t^8.98 - t^4.01/(g2*y) - t^5.02/(g2^2*y) - t^6.05/(g2^6*y) - (g2^8*t^6.94)/y - (g2^5*t^6.96)/y - (g2^2*t^6.98)/y - t^7.01/(g2*y) - t^7.03/(g2^4*y) - t^7.06/(g2^7*y) - (g2^7*t^7.94)/y + (g2^4*t^7.97)/y + t^8.06/(g2^8*y) - t^8.09/(g2^11*y) + (g2^15*t^8.88)/y + (g2^12*t^8.9)/y + (2*g2^9*t^8.93)/y + (g2^6*t^8.95)/y + (2*g2^3*t^8.98)/y - (t^4.01*y)/g2 - (t^5.02*y)/g2^2 - (t^6.05*y)/g2^6 - g2^8*t^6.94*y - g2^5*t^6.96*y - g2^2*t^6.98*y - (t^7.01*y)/g2 - (t^7.03*y)/g2^4 - (t^7.06*y)/g2^7 - g2^7*t^7.94*y + g2^4*t^7.97*y + (t^8.06*y)/g2^8 - (t^8.09*y)/g2^11 + g2^15*t^8.88*y + g2^12*t^8.9*y + 2*g2^9*t^8.93*y + g2^6*t^8.95*y + 2*g2^3*t^8.98*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 |
---|---|---|---|---|---|---|---|---|---|
57617 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}^{3}$ | 1.4537 | 1.644 | 0.8843 | [X:[1.3275], M:[0.9913], q:[0.4912, 0.4999], qb:[0.5088, 0.4826], phi:[0.3362]] | t^2.92 + t^2.95 + t^2.97 + t^3. + t^3.03 + t^3.93 + t^3.96 + t^3.98 + t^4.01 + t^4.03 + t^4.94 + t^4.97 + t^5.02 + t^5.04 + t^5.43 + t^5.46 + t^5.48 + t^5.51 + t^5.84 + t^5.87 + 2*t^5.9 + t^5.92 + 3*t^5.95 + t^5.97 - 2*t^6. - t^4.01/y - t^5.02/y - t^4.01*y - t^5.02*y | detail |