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 |
|---|---|---|---|---|---|---|---|---|---|
| 3852 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}X_{1}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{7}$ + ${ }M_{8}\phi_{1}^{2}$ | 0.6165 | 0.7524 | 0.8195 | [X:[1.6094], M:[0.8283, 0.7339, 1.1717, 0.3906, 0.8283, 0.7323, 1.2661, 1.2189], q:[0.3897, 0.7819], qb:[0.4386, 0.8275], phi:[0.3906]] | [X:[[0, 1]], M:[[0, 3], [0, -7], [0, -3], [0, -1], [0, 3], [2, -13], [0, 7], [0, 2]], q:[[1, -4], [-1, 1]], qb:[[-1, 7], [1, 0]], phi:[[0, -1]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{1}$, ${ }M_{5}$, ${ }\phi_{1}q_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{8}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{7}$, ${ }M_{6}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{5}M_{6}$, ${ }X_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{5}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{6}\phi_{1}q_{1}^{2}$, ${ }M_{6}q_{1}\tilde{q}_{2}$, ${ }M_{6}M_{8}$, ${ }M_{6}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{6}M_{7}$, ${ }M_{5}\phi_{1}q_{1}^{2}$ | ${}$ | -3 | t^2.197 + 2*t^2.485 + t^3.51 + t^3.652 + 2*t^3.657 + t^3.662 + t^3.798 + t^4.394 + 2*t^4.682 + t^4.828 + 3*t^4.97 + t^5.707 + t^5.849 + t^5.853 + 2*t^5.995 - 3*t^6. - t^6.005 + 2*t^6.137 + 3*t^6.142 + t^6.147 + 2*t^6.283 + t^6.591 + 2*t^6.879 + t^7.02 - t^7.03 + t^7.162 + 3*t^7.167 - 2*t^7.172 - t^7.177 + t^7.303 + 2*t^7.308 + 2*t^7.313 + t^7.323 + t^7.45 + 5*t^7.455 + t^7.596 + t^7.904 + t^8.045 + t^8.05 + 2*t^8.192 - 3*t^8.197 - t^8.202 + 2*t^8.333 + t^8.338 - t^8.343 + 3*t^8.48 - 6*t^8.485 - 2*t^8.49 + 3*t^8.622 + 4*t^8.627 + 3*t^8.768 + t^8.787 - t^4.172/y - t^6.369/y - t^6.657/y + (2*t^7.682)/y + t^7.687/y + t^7.97/y + t^7.975/y - t^8.565/y + t^8.707/y + t^8.849/y + t^8.853/y + t^8.858/y + (3*t^8.995)/y - t^4.172*y - t^6.369*y - t^6.657*y + 2*t^7.682*y + t^7.687*y + t^7.97*y + t^7.975*y - t^8.565*y + t^8.707*y + t^8.849*y + t^8.853*y + t^8.858*y + 3*t^8.995*y | (g1^2*t^2.197)/g2^13 + 2*g2^3*t^2.485 + (g1^2*t^3.51)/g2^9 + (g1^2*t^3.652)/g2^4 + 2*g2^2*t^3.657 + (g2^8*t^3.662)/g1^2 + g2^7*t^3.798 + (g1^4*t^4.394)/g2^26 + (2*g1^2*t^4.682)/g2^10 + g2*t^4.828 + 3*g2^6*t^4.97 + (g1^4*t^5.707)/g2^22 + (g1^4*t^5.849)/g2^17 + (g1^2*t^5.853)/g2^11 + (2*g1^2*t^5.995)/g2^6 - 3*t^6. - (g2^6*t^6.005)/g1^2 + (2*g1^2*t^6.137)/g2 + 3*g2^5*t^6.142 + (g2^11*t^6.147)/g1^2 + 2*g2^10*t^6.283 + (g1^6*t^6.591)/g2^39 + (2*g1^4*t^6.879)/g2^23 + (g1^4*t^7.02)/g2^18 - t^7.03/g2^6 + (g1^4*t^7.162)/g2^13 + (3*g1^2*t^7.167)/g2^7 - (2*t^7.172)/g2 - (g2^5*t^7.177)/g1^2 + (g1^4*t^7.303)/g2^8 + (2*g1^2*t^7.308)/g2^2 + 2*g2^4*t^7.313 + (g2^16*t^7.323)/g1^4 + g1^2*g2^3*t^7.45 + 5*g2^9*t^7.455 + g2^14*t^7.596 + (g1^6*t^7.904)/g2^35 + (g1^6*t^8.045)/g2^30 + (g1^4*t^8.05)/g2^24 + (2*g1^4*t^8.192)/g2^19 - (3*g1^2*t^8.197)/g2^13 - t^8.202/g2^7 + (2*g1^4*t^8.333)/g2^14 + (g1^2*t^8.338)/g2^8 - t^8.343/g2^2 + (3*g1^2*t^8.48)/g2^3 - 6*g2^3*t^8.485 - (2*g2^9*t^8.49)/g1^2 + 3*g1^2*g2^2*t^8.622 + 4*g2^8*t^8.627 + 3*g2^13*t^8.768 + (g1^8*t^8.787)/g2^52 - t^4.172/(g2*y) - (g1^2*t^6.369)/(g2^14*y) - (g2^2*t^6.657)/y + (2*g1^2*t^7.682)/(g2^10*y) + t^7.687/(g2^4*y) + (g2^6*t^7.97)/y + (g2^12*t^7.975)/(g1^2*y) - (g1^4*t^8.565)/(g2^27*y) + (g1^4*t^8.707)/(g2^22*y) + (g1^4*t^8.849)/(g2^17*y) + (g1^2*t^8.853)/(g2^11*y) + t^8.858/(g2^5*y) + (3*g1^2*t^8.995)/(g2^6*y) - (t^4.172*y)/g2 - (g1^2*t^6.369*y)/g2^14 - g2^2*t^6.657*y + (2*g1^2*t^7.682*y)/g2^10 + (t^7.687*y)/g2^4 + g2^6*t^7.97*y + (g2^12*t^7.975*y)/g1^2 - (g1^4*t^8.565*y)/g2^27 + (g1^4*t^8.707*y)/g2^22 + (g1^4*t^8.849*y)/g2^17 + (g1^2*t^8.853*y)/g2^11 + (t^8.858*y)/g2^5 + (3*g1^2*t^8.995*y)/g2^6 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 3377 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}X_{1}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{2}M_{7}$ | 0.6342 | 0.7831 | 0.8099 | [X:[1.6118], M:[0.8354, 0.7174, 1.1646, 0.3882, 0.8354, 0.7243, 1.2826], q:[0.3916, 0.773], qb:[0.4437, 0.8388], phi:[0.3882]] | t^2.173 + t^2.329 + 2*t^2.506 + t^3.514 + t^3.65 + t^3.671 + t^3.691 + t^3.848 + t^4.346 + t^4.502 + t^4.658 + 2*t^4.679 + 3*t^4.835 + 3*t^5.012 + t^5.687 + t^5.844 + t^5.864 - 2*t^6. - t^4.165/y - t^4.165*y | detail |