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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60062 | SU3adj1nf2 | ${}M_{1}\phi_{1}^{3}$ + ${ }q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | 1.4595 | 1.6711 | 0.8734 | [X:[], M:[0.9878], q:[0.4336, 0.4458], qb:[0.5664, 0.5298], phi:[0.3374]] | [X:[], M:[[9]], q:[[8], [-1]], qb:[[-8], [19]], phi:[[-3]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ | ${}\phi_{1}^{2}q_{1}q_{2}^{2}$ | 0 | t^2.02 + t^2.89 + t^2.93 + t^2.96 + t^3. + t^3.04 + t^3.9 + t^3.94 + t^4.01 + 2*t^4.05 + 2*t^4.91 + 3*t^4.95 + 2*t^4.99 + 2*t^5.02 + 2*t^5.06 + t^5.78 + t^5.82 + 2*t^5.85 + 2*t^5.89 + 4*t^5.93 + 3*t^5.96 + t^6.04 + 3*t^6.07 - t^6.11 + t^6.79 + 2*t^6.83 + 2*t^6.87 + 3*t^6.9 + 6*t^6.94 + 6*t^6.98 + 3*t^7.01 + 3*t^7.05 + 3*t^7.09 - t^7.12 + 4*t^7.8 + 5*t^7.84 + 6*t^7.88 + 6*t^7.91 + 8*t^7.95 + 5*t^7.99 + t^8.02 + t^8.06 + 4*t^8.1 - t^8.13 + t^8.67 + t^8.71 + 2*t^8.74 + 3*t^8.78 + 6*t^8.82 + 8*t^8.85 + 5*t^8.89 + 4*t^8.93 + 7*t^8.96 - t^4.01/y - t^5.02/y - t^6.04/y - t^6.9/y - t^6.94/y - t^6.98/y - t^7.01/y - (2*t^7.05)/y + t^7.99/y - t^8.06/y + t^8.82/y + t^8.85/y + (2*t^8.89)/y + t^8.93/y + t^8.96/y - t^4.01*y - t^5.02*y - t^6.04*y - t^6.9*y - t^6.94*y - t^6.98*y - t^7.01*y - 2*t^7.05*y + t^7.99*y - t^8.06*y + t^8.82*y + t^8.85*y + 2*t^8.89*y + t^8.93*y + t^8.96*y | t^2.02/g1^6 + g1^27*t^2.89 + g1^18*t^2.93 + g1^9*t^2.96 + t^3. + t^3.04/g1^9 + g1^24*t^3.9 + g1^15*t^3.94 + t^4.01/g1^3 + (2*t^4.05)/g1^12 + 2*g1^21*t^4.91 + 3*g1^12*t^4.95 + 2*g1^3*t^4.99 + (2*t^5.02)/g1^6 + (2*t^5.06)/g1^15 + g1^54*t^5.78 + g1^45*t^5.82 + 2*g1^36*t^5.85 + 2*g1^27*t^5.89 + 4*g1^18*t^5.93 + 3*g1^9*t^5.96 + t^6.04/g1^9 + (3*t^6.07)/g1^18 - t^6.11/g1^27 + g1^51*t^6.79 + 2*g1^42*t^6.83 + 2*g1^33*t^6.87 + 3*g1^24*t^6.9 + 6*g1^15*t^6.94 + 6*g1^6*t^6.98 + (3*t^7.01)/g1^3 + (3*t^7.05)/g1^12 + (3*t^7.09)/g1^21 - t^7.12/g1^30 + 4*g1^48*t^7.8 + 5*g1^39*t^7.84 + 6*g1^30*t^7.88 + 6*g1^21*t^7.91 + 8*g1^12*t^7.95 + 5*g1^3*t^7.99 + t^8.02/g1^6 + t^8.06/g1^15 + (4*t^8.1)/g1^24 - t^8.13/g1^33 + g1^81*t^8.67 + g1^72*t^8.71 + 2*g1^63*t^8.74 + 3*g1^54*t^8.78 + 6*g1^45*t^8.82 + 8*g1^36*t^8.85 + 5*g1^27*t^8.89 + 4*g1^18*t^8.93 + 7*g1^9*t^8.96 - t^4.01/(g1^3*y) - t^5.02/(g1^6*y) - t^6.04/(g1^9*y) - (g1^24*t^6.9)/y - (g1^15*t^6.94)/y - (g1^6*t^6.98)/y - t^7.01/(g1^3*y) - (2*t^7.05)/(g1^12*y) + (g1^3*t^7.99)/y - t^8.06/(g1^15*y) + (g1^45*t^8.82)/y + (g1^36*t^8.85)/y + (2*g1^27*t^8.89)/y + (g1^18*t^8.93)/y + (g1^9*t^8.96)/y - (t^4.01*y)/g1^3 - (t^5.02*y)/g1^6 - (t^6.04*y)/g1^9 - g1^24*t^6.9*y - g1^15*t^6.94*y - g1^6*t^6.98*y - (t^7.01*y)/g1^3 - (2*t^7.05*y)/g1^12 + g1^3*t^7.99*y - (t^8.06*y)/g1^15 + g1^45*t^8.82*y + g1^36*t^8.85*y + 2*g1^27*t^8.89*y + g1^18*t^8.93*y + g1^9*t^8.96*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 |
---|---|---|---|---|---|---|---|---|---|
57608 | SU3adj1nf2 | ${}M_{1}\phi_{1}^{3}$ + ${ }q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ | 1.4746 | 1.6852 | 0.875 | [X:[], M:[0.9914], q:[0.4913, 0.4999], qb:[0.5087, 0.4829], phi:[0.3362]] | t^2.02 + t^2.92 + t^2.95 + t^2.97 + t^3. + t^3.03 + t^3.93 + t^3.96 + t^4.01 + 2*t^4.03 + 2*t^4.94 + 2*t^4.97 + t^4.99 + 2*t^5.02 + 2*t^5.04 + t^5.43 + t^5.46 + t^5.48 + t^5.51 + t^5.85 + t^5.87 + 2*t^5.9 + t^5.92 + 4*t^5.95 + 2*t^5.97 - 2*t^6. - t^4.01/y - t^5.02/y - t^4.01*y - t^5.02*y | detail |