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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57834 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | 1.4589 | 1.6682 | 0.8746 | [X:[1.3291], M:[0.6773], q:[0.4366, 0.4494], qb:[0.5634, 0.5378], phi:[0.3355]] | [X:[[6]], M:[[-15]], q:[[11], [-7]], qb:[[-11], [25]], phi:[[-3]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$ | ${}$ | -1 | t^2.03 + t^2.92 + t^2.96 + t^3. + t^3.02 + t^3.04 + t^3.93 + t^3.99 + t^4.01 + t^4.04 + t^4.06 + t^4.94 + t^4.96 + 2*t^4.97 + t^4.99 + 2*t^5.01 + t^5.03 + 2*t^5.05 + t^5.07 + t^5.85 + t^5.88 + 2*t^5.92 + t^5.94 + 2*t^5.96 + 2*t^5.98 - t^6. + 3*t^6.02 + 2*t^6.04 + t^6.06 + t^6.08 + t^6.1 + t^6.85 + t^6.89 + t^6.91 + 2*t^6.93 + 3*t^6.95 + 2*t^6.97 + 3*t^6.99 + 3*t^7.01 + 4*t^7.03 + 2*t^7.04 + 3*t^7.06 + 2*t^7.08 + t^7.1 + 3*t^7.86 + t^7.88 + 3*t^7.9 + t^7.92 + 5*t^7.94 + t^7.96 + 5*t^7.97 + 3*t^7.99 + 5*t^8.01 + t^8.03 + 4*t^8.05 + 3*t^8.07 + 2*t^8.09 + t^8.11 + t^8.13 + t^8.77 + t^8.81 + 2*t^8.85 + 2*t^8.87 + 2*t^8.88 + 4*t^8.9 - t^8.92 + 6*t^8.94 + 7*t^8.98 - t^4.01/y - t^5.01/y - t^6.04/y - t^6.93/y - t^6.97/y - t^7.01/y - t^7.03/y - (2*t^7.04)/y - t^7.94/y + t^7.96/y + t^7.99/y - t^8.01/y + t^8.88/y + t^8.92/y + (2*t^8.96)/y + t^8.98/y - t^4.01*y - t^5.01*y - t^6.04*y - t^6.93*y - t^6.97*y - t^7.01*y - t^7.03*y - 2*t^7.04*y - t^7.94*y + t^7.96*y + t^7.99*y - t^8.01*y + t^8.88*y + t^8.92*y + 2*t^8.96*y + t^8.98*y | t^2.03/g1^15 + g1^36*t^2.92 + g1^18*t^2.96 + t^3. + t^3.02/g1^9 + t^3.04/g1^18 + g1^33*t^3.93 + g1^6*t^3.99 + t^4.01/g1^3 + t^4.04/g1^21 + t^4.06/g1^30 + g1^30*t^4.94 + g1^21*t^4.96 + 2*g1^12*t^4.97 + g1^3*t^4.99 + (2*t^5.01)/g1^6 + t^5.03/g1^15 + (2*t^5.05)/g1^24 + t^5.07/g1^33 + g1^72*t^5.85 + g1^54*t^5.88 + 2*g1^36*t^5.92 + g1^27*t^5.94 + 2*g1^18*t^5.96 + 2*g1^9*t^5.98 - t^6. + (3*t^6.02)/g1^9 + (2*t^6.04)/g1^18 + t^6.06/g1^27 + t^6.08/g1^36 + t^6.1/g1^45 + g1^69*t^6.85 + g1^51*t^6.89 + g1^42*t^6.91 + 2*g1^33*t^6.93 + 3*g1^24*t^6.95 + 2*g1^15*t^6.97 + 3*g1^6*t^6.99 + (3*t^7.01)/g1^3 + (4*t^7.03)/g1^12 + (2*t^7.04)/g1^21 + (3*t^7.06)/g1^30 + (2*t^7.08)/g1^39 + t^7.1/g1^48 + 3*g1^66*t^7.86 + g1^57*t^7.88 + 3*g1^48*t^7.9 + g1^39*t^7.92 + 5*g1^30*t^7.94 + g1^21*t^7.96 + 5*g1^12*t^7.97 + 3*g1^3*t^7.99 + (5*t^8.01)/g1^6 + t^8.03/g1^15 + (4*t^8.05)/g1^24 + (3*t^8.07)/g1^33 + (2*t^8.09)/g1^42 + t^8.11/g1^51 + t^8.13/g1^60 + g1^108*t^8.77 + g1^90*t^8.81 + 2*g1^72*t^8.85 + 2*g1^63*t^8.87 + 2*g1^54*t^8.88 + 4*g1^45*t^8.9 - g1^36*t^8.92 + 6*g1^27*t^8.94 + 7*g1^9*t^8.98 - t^4.01/(g1^3*y) - t^5.01/(g1^6*y) - t^6.04/(g1^18*y) - (g1^33*t^6.93)/y - (g1^15*t^6.97)/y - t^7.01/(g1^3*y) - t^7.03/(g1^12*y) - (2*t^7.04)/(g1^21*y) - (g1^30*t^7.94)/y + (g1^21*t^7.96)/y + (g1^3*t^7.99)/y - t^8.01/(g1^6*y) + (g1^54*t^8.88)/y + (g1^36*t^8.92)/y + (2*g1^18*t^8.96)/y + (g1^9*t^8.98)/y - (t^4.01*y)/g1^3 - (t^5.01*y)/g1^6 - (t^6.04*y)/g1^18 - g1^33*t^6.93*y - g1^15*t^6.97*y - (t^7.01*y)/g1^3 - (t^7.03*y)/g1^12 - (2*t^7.04*y)/g1^21 - g1^30*t^7.94*y + g1^21*t^7.96*y + g1^3*t^7.99*y - (t^8.01*y)/g1^6 + g1^54*t^8.88*y + g1^36*t^8.92*y + 2*g1^18*t^8.96*y + g1^9*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 |
---|---|---|---|---|---|---|---|---|---|
57274 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$ | 1.474 | 1.6826 | 0.876 | [X:[1.3323], M:[0.6693], q:[0.4977, 0.5008], qb:[0.5023, 0.4961], phi:[0.3339]] | t^2.008 + t^2.981 + t^2.991 + t^3. + t^3.005 + t^3.009 + t^3.983 + t^3.997 + t^4.002 + t^4.011 + t^4.016 + t^4.984 + t^4.989 + t^4.994 + t^4.998 + t^5.003 + t^5.008 + 2*t^5.012 + t^5.017 + t^5.485 + t^5.49 + t^5.499 + t^5.504 + t^5.963 + t^5.972 + t^5.981 + t^5.986 + 2*t^5.991 + t^5.995 - 2*t^6. - t^4.002/y - t^5.003/y - t^4.002*y - t^5.003*y | detail |