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 |
|---|---|---|---|---|---|---|---|---|---|
| 58905 | SU3adj1nf2 | ${}M_{1}\phi_{1}^{3}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ | 1.4535 | 1.6403 | 0.8861 | [X:[1.3373], M:[1.006, 0.982], q:[0.5151, 0.4911], qb:[0.5029, 0.5029], phi:[0.3313]] | [X:[[0, 2]], M:[[0, 3], [0, -9]], q:[[-1, 9], [-1, -3]], qb:[[1, 0], [1, 0]], phi:[[0, -1]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$ | ${}$ | -3 | t^2.95 + 2*t^2.98 + t^3.02 + t^3.05 + 2*t^3.98 + t^4.01 + 2*t^4.05 + 2*t^4.97 + 2*t^5.04 + t^5.49 + 2*t^5.52 + t^5.56 + t^5.89 + t^5.93 + 4*t^5.96 - 3*t^6. + 3*t^6.04 + t^6.11 + t^6.48 + 2*t^6.51 + t^6.55 + t^6.92 + 5*t^6.96 + t^6.99 + 7*t^7.03 + 2*t^7.07 + 2*t^7.1 + t^7.4 + 2*t^7.51 - t^7.54 + t^7.55 + t^7.62 + t^7.92 + 7*t^7.95 + 10*t^8.02 + t^8.06 + 5*t^8.1 - t^8.43 + 2*t^8.5 + t^8.54 + 2*t^8.57 - t^8.58 + t^8.61 + t^8.84 + t^8.87 + 2*t^8.91 + 6*t^8.95 - 6*t^8.98 + t^8.98/y^2 - t^3.99/y - t^4.99/y - t^6.94/y - (2*t^6.98)/y - t^7.01/y - t^7.05/y - t^7.93/y - (2*t^7.97)/y - t^8.01/y - t^8.04/y + (2*t^8.93)/y - t^3.99*y - t^4.99*y - t^6.94*y - 2*t^6.98*y - t^7.01*y - t^7.05*y - t^7.93*y - 2*t^7.97*y - t^8.01*y - t^8.04*y + 2*t^8.93*y + t^8.98*y^2 | t^2.95/g2^9 + (2*t^2.98)/g2^3 + g2^3*t^3.02 + g2^9*t^3.05 + (2*t^3.98)/g2^4 + g2^2*t^4.01 + 2*g2^8*t^4.05 + (2*t^4.97)/g2^5 + 2*g2^7*t^5.04 + (g2^2*t^5.49)/g1^3 + (2*g1^3*t^5.52)/g2 + (g2^14*t^5.56)/g1^3 + t^5.89/g2^18 + t^5.93/g2^12 + (4*t^5.96)/g2^6 - 3*t^6. + 3*g2^6*t^6.04 + g2^18*t^6.11 + (g2*t^6.48)/g1^3 + (2*g1^3*t^6.51)/g2^2 + (g2^13*t^6.55)/g1^3 + t^6.92/g2^13 + (5*t^6.96)/g2^7 + t^6.99/g2 + 7*g2^5*t^7.03 + 2*g2^11*t^7.07 + 2*g2^17*t^7.1 + t^7.4/(g1^3*g2^12) + t^7.47/g1^3 - (g1^3*t^7.47)/g2^9 + (4*g1^3*t^7.51)/g2^3 - (2*g2^6*t^7.51)/g1^3 - g1^3*g2^3*t^7.54 + (g2^12*t^7.55)/g1^3 + (g2^24*t^7.62)/g1^3 + t^7.92/g2^14 + (7*t^7.95)/g2^8 + 10*g2^4*t^8.02 + g2^10*t^8.06 + 5*g2^16*t^8.1 - t^8.43/(g1^3*g2^7) - (2*g1^3*t^8.47)/g2^10 + (2*t^8.47)/(g1^3*g2) + (4*g1^3*t^8.5)/g2^4 - (2*g2^5*t^8.5)/g1^3 - 2*g1^3*g2^2*t^8.54 + (3*g2^11*t^8.54)/g1^3 + 2*g1^3*g2^8*t^8.57 - (g2^17*t^8.58)/g1^3 + (g2^23*t^8.61)/g1^3 + t^8.84/g2^27 + t^8.87/g2^21 + (2*t^8.91)/g2^15 + (6*t^8.95)/g2^9 - (6*t^8.98)/g2^3 + t^8.98/(g2^3*y^2) - t^3.99/(g2*y) - t^4.99/(g2^2*y) - t^6.94/(g2^10*y) - (2*t^6.98)/(g2^4*y) - (g2^2*t^7.01)/y - (g2^8*t^7.05)/y - t^7.93/(g2^11*y) - (2*t^7.97)/(g2^5*y) - (g2*t^8.01)/y - (g2^7*t^8.04)/y + (2*t^8.93)/(g2^12*y) - (t^3.99*y)/g2 - (t^4.99*y)/g2^2 - (t^6.94*y)/g2^10 - (2*t^6.98*y)/g2^4 - g2^2*t^7.01*y - g2^8*t^7.05*y - (t^7.93*y)/g2^11 - (2*t^7.97*y)/g2^5 - g2*t^8.01*y - g2^7*t^8.04*y + (2*t^8.93*y)/g2^12 + (t^8.98*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 |
|---|---|---|---|---|---|---|---|---|---|
| 57479 | SU3adj1nf2 | ${}M_{1}\phi_{1}^{3}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ | 1.4758 | 1.6871 | 0.8747 | [X:[], M:[0.9966, 0.9668], q:[0.5131, 0.4833], qb:[0.5201, 0.4768], phi:[0.3345]] | t^2.01 + t^2.88 + t^2.9 + t^2.97 + t^2.99 + t^3.01 + t^3.88 + t^3.97 + 2*t^4.01 + t^4.1 + 2*t^4.89 + t^4.91 + 2*t^4.98 + t^5. + 2*t^5.02 + t^5.11 + t^5.42 + t^5.44 + t^5.53 + t^5.55 + t^5.76 + t^5.78 + t^5.8 + t^5.85 + t^5.87 + 3*t^5.89 + t^5.94 + t^5.96 + 3*t^5.98 - 3*t^6. - t^4./y - t^5.01/y - t^4.*y - t^5.01*y | detail |