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 |
---|---|---|---|---|---|---|---|---|---|
58181 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{1}$ | 1.4759 | 1.6818 | 0.8775 | [X:[1.3441], M:[0.9514, 0.6883], q:[0.4919, 0.5243], qb:[0.4919, 0.5243], phi:[0.3279]] | [X:[[0, 2]], M:[[0, -9], [0, 4]], q:[[-1, 3], [-1, 9]], qb:[[1, -6], [1, 0]], phi:[[0, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{2}$, ${ }M_{1}$, ${ }\phi_{1}^{3}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }M_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }M_{2}\phi_{1}^{3}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{6}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ }M_{1}q_{1}\tilde{q}_{2}$ | ${}\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ | 0 | t^2.06 + t^2.85 + 2*t^2.95 + 2*t^3.05 + 3*t^4.03 + 2*t^4.13 + 2*t^4.92 + 4*t^5.02 + 3*t^5.11 + 2*t^5.51 + 2*t^5.61 + t^5.71 + 2*t^5.81 + 3*t^5.9 + 4*t^6.1 + 2*t^6.19 + 2*t^6.49 + 2*t^6.59 + t^6.89 + 6*t^6.98 + 10*t^7.08 + 5*t^7.18 + 2*t^7.38 + 2*t^7.57 + 4*t^7.67 + 2*t^7.77 + 4*t^7.87 + 7*t^7.97 + 7*t^8.06 + 8*t^8.16 + 3*t^8.26 + 5*t^8.56 + 4*t^8.65 + 2*t^8.66 + 3*t^8.76 + t^8.85 + t^8.95 + t^8.95/y^2 - t^3.98/y - t^4.97/y - t^6.05/y - t^6.84/y - (2*t^6.94)/y - (3*t^7.03)/y - t^7.82/y + t^8.11/y + (2*t^8.81)/y + (2*t^8.9)/y - t^3.98*y - t^4.97*y - t^6.05*y - t^6.84*y - 2*t^6.94*y - 3*t^7.03*y - t^7.82*y + t^8.11*y + 2*t^8.81*y + 2*t^8.9*y + t^8.95*y^2 | g2^4*t^2.06 + t^2.85/g2^9 + (2*t^2.95)/g2^3 + 2*g2^3*t^3.05 + 3*g2^2*t^4.03 + 2*g2^8*t^4.13 + (2*t^4.92)/g2^5 + 4*g2*t^5.02 + 3*g2^7*t^5.11 + (g1^3*t^5.51)/g2^13 + (g2^14*t^5.51)/g1^3 + (g1^3*t^5.61)/g2^7 + (g2^20*t^5.61)/g1^3 + t^5.71/g2^18 + (2*t^5.81)/g2^12 + (3*t^5.9)/g2^6 + 4*g2^6*t^6.1 + 2*g2^12*t^6.19 + (g1^3*t^6.49)/g2^14 + (g2^13*t^6.49)/g1^3 + (g1^3*t^6.59)/g2^8 + (g2^19*t^6.59)/g1^3 + t^6.89/g2^7 + (6*t^6.98)/g2 + 10*g2^5*t^7.08 + 5*g2^11*t^7.18 + (g1^3*t^7.38)/g2^21 + (g2^6*t^7.38)/g1^3 + (g1^3*t^7.57)/g2^9 + (g2^18*t^7.57)/g1^3 + (2*g1^3*t^7.67)/g2^3 + (2*g2^24*t^7.67)/g1^3 + (2*t^7.77)/g2^14 + (4*t^7.87)/g2^8 + (7*t^7.97)/g2^2 + 7*g2^4*t^8.06 + 8*g2^10*t^8.16 + 3*g2^16*t^8.26 + t^8.56/g2^27 + (2*g1^3*t^8.56)/g2^10 + (2*g2^17*t^8.56)/g1^3 + (2*g1^3*t^8.65)/g2^4 + (2*g2^23*t^8.65)/g1^3 + (2*t^8.66)/g2^21 + (3*t^8.76)/g2^15 + t^8.85/g2^9 + t^8.95/g2^3 + t^8.95/(g2^3*y^2) - t^3.98/(g2*y) - t^4.97/(g2^2*y) - (g2^3*t^6.05)/y - t^6.84/(g2^10*y) - (2*t^6.94)/(g2^4*y) - (3*g2^2*t^7.03)/y - t^7.82/(g2^11*y) + (g2^7*t^8.11)/y + (2*t^8.81)/(g2^12*y) + (2*t^8.9)/(g2^6*y) - (t^3.98*y)/g2 - (t^4.97*y)/g2^2 - g2^3*t^6.05*y - (t^6.84*y)/g2^10 - (2*t^6.94*y)/g2^4 - 3*g2^2*t^7.03*y - (t^7.82*y)/g2^11 + g2^7*t^8.11*y + (2*t^8.81*y)/g2^12 + (2*t^8.9*y)/g2^6 + (t^8.95*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 |
---|
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 |
---|
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 |
---|
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 |
---|---|---|---|---|---|---|---|---|---|
57273 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$ | 1.4552 | 1.6416 | 0.8864 | [X:[1.3449], M:[0.948], q:[0.4913, 0.526], qb:[0.4913, 0.526], phi:[0.3276]] | t^2.844 + 2*t^2.948 + 2*t^3.052 + t^3.931 + 3*t^4.035 + t^4.139 + t^4.913 + 2*t^5.017 + t^5.121 + 2*t^5.509 + 2*t^5.613 + t^5.688 + 2*t^5.792 + 3*t^5.896 - t^3.983/y - t^4.965/y - t^3.983*y - t^4.965*y | detail |