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 |
|---|---|---|---|---|---|---|---|---|---|
| 58154 | SU3adj1nf2 | ${}M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{6}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ | 1.4437 | 1.6353 | 0.8828 | [X:[1.3333], M:[0.9346, 0.9988], q:[0.577, 0.5128], qb:[0.4885, 0.4218], phi:[0.3333]] | [X:[[0, 0]], M:[[-2, -1], [1, 2]], q:[[1, 1], [-2, -2]], qb:[[1, 0], [0, 1]], phi:[[0, 0]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}^{3}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$ | ${}M_{2}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | 1 | 2*t^2.8 + 3*t^3. + t^3.8 + 3*t^4. + t^4.2 + t^4.8 + 3*t^5. + 2*t^5.2 + 3*t^5.61 + 5*t^5.8 + 3*t^5.99 + t^6. - t^6.19 + 2*t^6.61 + 7*t^6.8 + 2*t^6.81 + 2*t^6.99 + 7*t^7. + t^7.2 + t^7.4 + 4*t^7.61 + 5*t^7.8 + 3*t^7.81 + 4*t^7.99 + 7*t^8. + t^8.01 + 3*t^8.19 + t^8.2 + 4*t^8.41 + 4*t^8.6 + 3*t^8.61 + 6*t^8.8 + t^8.81 + 10*t^8.99 - t^4./y - t^5./y - (2*t^6.8)/y - (3*t^7.)/y - (2*t^7.8)/y - (3*t^8.)/y + t^8.61/y + (5*t^8.8)/y + t^8.99/y - t^4.*y - t^5.*y - 2*t^6.8*y - 3*t^7.*y - 2*t^7.8*y - 3*t^8.*y + t^8.61*y + 5*t^8.8*y + t^8.99*y | (2*t^2.8)/(g1^2*g2) + t^3. + 2*g1*g2^2*t^3. + t^3.8/(g1^2*g2) + t^4. + t^4./(g1*g2^2) + g1*g2^2*t^4. + g1^2*g2*t^4.2 + t^4.8/(g1^2*g2) + t^5./(g1*g2^2) + 2*g1*g2^2*t^5. + 2*g1^2*g2*t^5.2 + (3*t^5.61)/(g1^4*g2^2) + (2*t^5.8)/(g1^2*g2) + (3*g2*t^5.8)/g1 + 3*g1^2*g2^4*t^5.99 - 2*t^6. + 3*g1*g2^2*t^6. - g1^3*g2^3*t^6.19 - (g1*t^6.2)/g2 + g1^2*g2*t^6.2 + (2*t^6.61)/(g1^4*g2^2) + (3*t^6.8)/(g1^2*g2) + (3*g2*t^6.8)/g1 + g2^3*t^6.8 + (2*t^6.81)/(g1^3*g2^3) + 2*g1^2*g2^4*t^6.99 + 2*t^7. + t^7./(g1*g2^2) + 4*g1*g2^2*t^7. - (g1*t^7.2)/g2 + 2*g1^2*g2*t^7.2 + g1^3*t^7.4 + t^7.61/(g1^6*g2^6) + (3*t^7.61)/(g1^4*g2^2) + (5*g2*t^7.8)/g1 + (3*t^7.81)/(g1^3*g2^3) + 4*g1^2*g2^4*t^7.99 + 5*t^8. + 2*g1*g2^2*t^8. + t^8.01/(g1^2*g2^4) + 3*g1^3*g2^3*t^8.19 - (g1*t^8.2)/g2 + 2*g1^2*g2*t^8.2 + (4*t^8.41)/(g1^6*g2^3) + (4*t^8.6)/g1^3 - t^8.61/(g1^5*g2^4) + (4*t^8.61)/(g1^4*g2^2) - (5*t^8.8)/(g1^2*g2) + (7*g2*t^8.8)/g1 + 4*g2^3*t^8.8 - t^8.81/(g1^4*g2^5) + (2*t^8.81)/(g1^3*g2^3) + 6*g1^2*g2^4*t^8.99 + 4*g1^3*g2^6*t^8.99 - t^4./y - t^5./y - (2*t^6.8)/(g1^2*g2*y) - t^7./y - (2*g1*g2^2*t^7.)/y - (2*t^7.8)/(g1^2*g2*y) - t^8./y - (2*g1*g2^2*t^8.)/y + t^8.61/(g1^4*g2^2*y) + t^8.8/(g1^2*g2*y) + (4*g2*t^8.8)/(g1*y) + (g1^2*g2^4*t^8.99)/y - t^4.*y - t^5.*y - (2*t^6.8*y)/(g1^2*g2) - t^7.*y - 2*g1*g2^2*t^7.*y - (2*t^7.8*y)/(g1^2*g2) - t^8.*y - 2*g1*g2^2*t^8.*y + (t^8.61*y)/(g1^4*g2^2) + (t^8.8*y)/(g1^2*g2) + (4*g2*t^8.8*y)/g1 + g1^2*g2^4*t^8.99*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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 57338 | SU3adj1nf2 | ${}M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}^{6}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ | 1.4566 | 1.6487 | 0.8835 | [X:[1.3333], M:[0.9634, 0.9634], q:[0.4993, 0.4993], qb:[0.5373, 0.464], phi:[0.3333]] | 4*t^2.89 + t^3. + 2*t^3.89 + t^4. + 2*t^4.11 + 2*t^4.89 + 2*t^5.11 + t^5.396 + 2*t^5.494 + t^5.616 + 9*t^5.78 + 4*t^5.89 - 5*t^6. - t^4./y - t^5./y - t^4.*y - t^5.*y | detail |