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 |
|---|---|---|---|---|---|---|---|---|---|
| 58808 | SU3adj1nf2 | ${}M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }q_{1}^{2}\tilde{q}_{2}^{2}$ | 1.4532 | 1.6401 | 0.886 | [X:[1.3353], M:[1.0029, 0.9941], q:[0.4971, 0.5059], qb:[0.5, 0.5029], phi:[0.3324]] | [X:[[0, 2]], M:[[0, 3], [0, -6]], q:[[-1, 0], [-1, 9]], qb:[[1, -3], [1, 0]], phi:[[0, -1]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }\phi_{1}^{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}^{6}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$ | ${}$ | -2 | t^2.98 + t^2.99 + t^3. + t^3.01 + t^3.03 + t^3.99 + t^4. + 2*t^4.01 + t^4.02 + 2*t^4.99 + t^5.01 + t^5.02 + t^5.5 + 2*t^5.51 + t^5.52 + t^5.96 + 2*t^5.98 + t^5.99 - 2*t^6. + t^6.01 + 2*t^6.02 + t^6.04 + t^6.05 + t^6.49 + t^6.5 + t^6.51 + t^6.52 + 2*t^6.98 + 2*t^6.99 + t^7. + 7*t^7.01 + 2*t^7.02 + 2*t^7.03 + t^7.04 + t^7.05 + t^7.46 + t^7.49 + t^7.52 + t^7.54 + 3*t^7.98 + 4*t^7.99 + 3*t^8. + 5*t^8.01 + 3*t^8.02 + 2*t^8.03 + 2*t^8.04 + 2*t^8.05 - t^8.47 - t^8.48 + 2*t^8.51 + t^8.52 + t^8.53 + t^8.54 + t^8.55 + t^8.95 + t^8.96 + 3*t^8.97 + t^8.99/y^2 - t^4./y - t^4.99/y - t^6.98/y - t^6.99/y - t^7./y - t^7.01/y - t^7.02/y - t^7.98/y - (2*t^7.99)/y - t^8./y - t^8.02/y + t^8.97/y + t^8.99/y - t^4.*y - t^4.99*y - t^6.98*y - t^6.99*y - t^7.*y - t^7.01*y - t^7.02*y - t^7.98*y - 2*t^7.99*y - t^8.*y - t^8.02*y + t^8.97*y + t^8.99*y + t^8.99*y^2 | t^2.98/g2^6 + t^2.99/g2^3 + t^3. + g2^3*t^3.01 + g2^9*t^3.03 + t^3.99/g2^4 + t^4./g2 + g2^2*t^4.01 + g2^5*t^4.01 + g2^8*t^4.02 + t^4.99/g2^5 + t^4.99/g2^2 + g2^4*t^5.01 + g2^7*t^5.02 + (g2^8*t^5.5)/g1^3 + (g1^3*t^5.51)/g2^7 + (g1^3*t^5.51)/g2^4 + (g2^17*t^5.52)/g1^3 + t^5.96/g2^12 + (2*t^5.98)/g2^6 + t^5.99/g2^3 - 2*t^6. + g2^3*t^6.01 + 2*g2^6*t^6.02 + g2^12*t^6.04 + g2^18*t^6.05 + (g2^7*t^6.49)/g1^3 + (g1^3*t^6.5)/g2^8 + (g1^3*t^6.51)/g2^5 + (g2^16*t^6.52)/g1^3 + (2*t^6.98)/g2^7 + (2*t^6.99)/g2^4 + t^7./g2 + 3*g2^2*t^7.01 + 4*g2^5*t^7.01 + 2*g2^8*t^7.02 + 2*g2^11*t^7.03 + g2^14*t^7.04 + g2^17*t^7.05 + t^7.46/(g1^3*g2^3) + (g2^6*t^7.49)/g1^3 + (g1^3*t^7.5)/g2^9 - (g2^9*t^7.5)/g1^3 + (g1^3*t^7.51)/g2^6 - (g2^12*t^7.51)/g1^3 + (g2^15*t^7.52)/g1^3 + (g2^24*t^7.54)/g1^3 + (3*t^7.98)/g2^8 + (2*t^7.99)/g2^5 + (2*t^7.99)/g2^2 + 3*g2*t^8. + 5*g2^4*t^8.01 + 3*g2^7*t^8.02 + 2*g2^10*t^8.03 + 2*g2^13*t^8.04 + 2*g2^16*t^8.05 - t^8.47/(g1^3*g2) - (g1^3*t^8.48)/g2^16 - (g1^3*t^8.49)/g2^13 + (g2^5*t^8.49)/g1^3 + (g1^3*t^8.5)/g2^10 - (g2^8*t^8.5)/g1^3 + (g1^3*t^8.51)/g2^7 + (g2^14*t^8.51)/g1^3 + (g2^17*t^8.52)/g1^3 + g1^3*g2^2*t^8.53 + g1^3*g2^5*t^8.54 + (g2^26*t^8.55)/g1^3 + t^8.95/g2^18 + t^8.96/g2^12 + (3*t^8.97)/g2^9 + t^8.99/(g2^3*y^2) - t^4./(g2*y) - t^4.99/(g2^2*y) - t^6.98/(g2^7*y) - t^6.99/(g2^4*y) - t^7./(g2*y) - (g2^2*t^7.01)/y - (g2^8*t^7.02)/y - t^7.98/(g2^8*y) - t^7.99/(g2^5*y) - t^7.99/(g2^2*y) - (g2*t^8.)/y - (g2^7*t^8.02)/y + t^8.97/(g2^9*y) + t^8.99/(g2^3*y) - (t^4.*y)/g2 - (t^4.99*y)/g2^2 - (t^6.98*y)/g2^7 - (t^6.99*y)/g2^4 - (t^7.*y)/g2 - g2^2*t^7.01*y - g2^8*t^7.02*y - (t^7.98*y)/g2^8 - (t^7.99*y)/g2^5 - (t^7.99*y)/g2^2 - g2*t^8.*y - g2^7*t^8.02*y + (t^8.97*y)/g2^9 + (t^8.99*y)/g2^3 + (t^8.99*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 |
|---|---|---|---|---|---|---|---|---|---|
| 57467 | SU3adj1nf2 | ${}M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{1}\phi_{1}^{3}$ | 1.4549 | 1.6456 | 0.8841 | [X:[1.331], M:[0.9966, 0.9669], q:[0.4833, 0.513], qb:[0.5201, 0.4767], phi:[0.3345]] | t^2.88 + t^2.9 + t^2.97 + t^2.99 + t^3.01 + t^3.88 + t^3.97 + t^3.99 + t^4.01 + t^4.1 + t^4.89 + t^4.98 + 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 + 2*t^5.89 + t^5.94 + t^5.96 + 2*t^5.98 - 3*t^6. - t^4./y - t^5.01/y - t^4.*y - t^5.01*y | detail |