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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58110 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}X_{1}$ | 1.4749 | 1.6859 | 0.8748 | [X:[1.328], M:[0.984, 0.672], q:[0.4879, 0.5039], qb:[0.5121, 0.48], phi:[0.336]] | [X:[[0, 2]], M:[[0, 6], [0, -2]], q:[[-1, 12], [-1, 6]], qb:[[1, -12], [1, 0]], phi:[[0, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }M_{2}\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}^{3}$, ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$ | ${}$ | -3 | t^2.02 + t^2.9 + 2*t^2.95 + t^3. + t^3.02 + t^3.91 + t^3.96 + t^4.01 + t^4.03 + t^4.06 + 2*t^4.92 + 3*t^4.97 + 2*t^5.02 + t^5.04 + t^5.06 + t^5.42 + t^5.45 + t^5.5 + t^5.52 + t^5.81 + 2*t^5.86 + 3*t^5.9 + 2*t^5.93 + t^5.95 + 3*t^5.98 - 3*t^6. + 2*t^6.02 + t^6.05 + t^6.07 - t^6.1 + t^6.43 + t^6.46 + t^6.5 + t^6.53 + t^6.82 + 3*t^6.86 + 3*t^6.91 + 3*t^6.94 + 3*t^6.96 + 4*t^6.98 + 3*t^7.03 + t^7.06 + 2*t^7.08 - t^7.1 + t^7.34 + t^7.41 + t^7.44 + t^7.46 + t^7.51 + t^7.54 + t^7.56 + t^7.63 + 3*t^7.82 + 6*t^7.87 - t^7.9 + 8*t^7.92 + 2*t^7.94 + 5*t^7.97 + 3*t^7.99 + 2*t^8.04 + 2*t^8.06 + 2*t^8.09 - t^8.11 + t^8.33 + t^8.35 + t^8.38 + 2*t^8.4 + t^8.42 + 3*t^8.45 + 2*t^8.47 - t^8.5 + t^8.52 - t^8.57 - t^8.59 - t^8.62 + t^8.71 + 2*t^8.76 + 3*t^8.81 + 3*t^8.83 + 3*t^8.86 + 7*t^8.88 - 4*t^8.9 + 9*t^8.93 - 4*t^8.95 + 7*t^8.98 - t^4.01/y - t^5.02/y - t^6.02/y - t^6.91/y - (2*t^6.96)/y - t^7.01/y - (2*t^7.03)/y + t^7.99/y - t^8.04/y + (2*t^8.86)/y + (2*t^8.9)/y + (2*t^8.95)/y - t^4.01*y - t^5.02*y - t^6.02*y - t^6.91*y - 2*t^6.96*y - t^7.01*y - 2*t^7.03*y + t^7.99*y - t^8.04*y + 2*t^8.86*y + 2*t^8.9*y + 2*t^8.95*y | t^2.02/g2^2 + g2^12*t^2.9 + 2*g2^6*t^2.95 + t^3. + t^3.02/g2^3 + g2^11*t^3.91 + g2^5*t^3.96 + t^4.01/g2 + t^4.03/g2^4 + t^4.06/g2^7 + 2*g2^10*t^4.92 + 3*g2^4*t^4.97 + (2*t^5.02)/g2^2 + t^5.04/g2^5 + t^5.06/g2^8 + (g1^3*t^5.42)/g2^13 + (g2^29*t^5.45)/g1^3 + (g2^23*t^5.5)/g1^3 + (g1^3*t^5.52)/g2^25 + g2^24*t^5.81 + 2*g2^18*t^5.86 + 3*g2^12*t^5.9 + 2*g2^9*t^5.93 + g2^6*t^5.95 + 3*g2^3*t^5.98 - 3*t^6. + (2*t^6.02)/g2^3 + t^6.05/g2^6 + t^6.07/g2^9 - t^6.1/g2^12 + (g1^3*t^6.43)/g2^14 + (g2^28*t^6.46)/g1^3 + (g2^22*t^6.5)/g1^3 + (g1^3*t^6.53)/g2^26 + g2^23*t^6.82 + 3*g2^17*t^6.86 + 3*g2^11*t^6.91 + 3*g2^8*t^6.94 + 3*g2^5*t^6.96 + 4*g2^2*t^6.98 + (3*t^7.03)/g2^4 + t^7.06/g2^7 + (2*t^7.08)/g2^10 - t^7.1/g2^13 + (g1^3*t^7.34)/g2^3 + (g2^33*t^7.41)/g1^3 + (2*g1^3*t^7.44)/g2^15 - (g2^30*t^7.44)/g1^3 - (g1^3*t^7.46)/g2^18 + (2*g2^27*t^7.46)/g1^3 - (g1^3*t^7.51)/g2^24 + (2*g2^21*t^7.51)/g1^3 + (2*g1^3*t^7.54)/g2^27 - (g2^18*t^7.54)/g1^3 + (g2^15*t^7.56)/g1^3 + (g1^3*t^7.63)/g2^39 + 3*g2^22*t^7.82 + 6*g2^16*t^7.87 - g2^13*t^7.9 + 8*g2^10*t^7.92 + 2*g2^7*t^7.94 + 5*g2^4*t^7.97 + 3*g2*t^7.99 + (2*t^8.04)/g2^5 + (2*t^8.06)/g2^8 + (2*t^8.09)/g2^11 - t^8.11/g2^14 + (g1^3*t^8.33)/g2 + (g2^41*t^8.35)/g1^3 + (g1^3*t^8.38)/g2^7 + (2*g2^35*t^8.4)/g1^3 + (g1^3*t^8.42)/g2^13 + (2*g1^3*t^8.45)/g2^16 + (g2^29*t^8.45)/g1^3 + (2*g2^26*t^8.47)/g1^3 - (g2^23*t^8.5)/g1^3 - (g1^3*t^8.52)/g2^25 + (2*g2^20*t^8.52)/g1^3 + (2*g1^3*t^8.54)/g2^28 - (2*g2^17*t^8.54)/g1^3 - (g1^3*t^8.57)/g2^31 - (g2^11*t^8.59)/g1^3 - (g1^3*t^8.62)/g2^37 + g2^36*t^8.71 + 2*g2^30*t^8.76 + 3*g2^24*t^8.81 + 3*g2^21*t^8.83 + 3*g2^18*t^8.86 + 7*g2^15*t^8.88 - 4*g2^12*t^8.9 + 9*g2^9*t^8.93 - 4*g2^6*t^8.95 + 7*g2^3*t^8.98 - t^4.01/(g2*y) - t^5.02/(g2^2*y) - t^6.02/(g2^3*y) - (g2^11*t^6.91)/y - (2*g2^5*t^6.96)/y - t^7.01/(g2*y) - (2*t^7.03)/(g2^4*y) + (g2*t^7.99)/y - t^8.04/(g2^5*y) + (2*g2^18*t^8.86)/y + (2*g2^12*t^8.9)/y + (2*g2^6*t^8.95)/y - (t^4.01*y)/g2 - (t^5.02*y)/g2^2 - (t^6.02*y)/g2^3 - g2^11*t^6.91*y - 2*g2^5*t^6.96*y - (t^7.01*y)/g2 - (2*t^7.03*y)/g2^4 + g2*t^7.99*y - (t^8.04*y)/g2^5 + 2*g2^18*t^8.86*y + 2*g2^12*t^8.9*y + 2*g2^6*t^8.95*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 |
---|---|---|---|---|---|---|---|---|---|
57335 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ | 1.4541 | 1.6446 | 0.8841 | [X:[1.3279], M:[0.9838], q:[0.4878, 0.5039], qb:[0.5122, 0.4799], phi:[0.336]] | t^2.903 + 2*t^2.951 + t^3. + t^3.024 + t^3.911 + t^3.96 + t^3.984 + t^4.008 + t^4.057 + t^4.919 + t^4.968 + t^5.016 + t^5.065 + t^5.424 + t^5.447 + t^5.495 + t^5.521 + t^5.806 + 2*t^5.854 + 3*t^5.903 + t^5.927 + t^5.951 + 2*t^5.976 - 3*t^6. - t^4.008/y - t^5.016/y - t^4.008*y - t^5.016*y | detail |