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 |
|---|---|---|---|---|---|---|---|---|---|
| 47127 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{1}M_{5}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}$ + ${ }q_{1}^{2}\tilde{q}_{2}^{2}$ + ${ }M_{3}X_{1}$ | 0.6768 | 0.8295 | 0.8159 | [X:[1.3406], M:[1.1135, 0.7838, 0.6594, 0.9891, 0.8865], q:[0.4378, 0.4487], qb:[0.7784, 0.5622], phi:[0.4432]] | [X:[[12]], M:[[4], [10], [-12], [-18], [-4]], q:[[-11], [7]], qb:[[1], [11]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }M_{4}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}M_{4}$, ${ }M_{5}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}M_{5}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$ | ${}$ | -2 | t^2.351 + 2*t^2.659 + t^2.967 + t^3. + t^3.681 + t^3.957 + t^3.989 + 2*t^4.022 + t^4.33 + t^4.362 + 2*t^4.703 + 2*t^5.011 + 4*t^5.319 + t^5.351 + t^5.627 + t^5.659 + t^5.935 - 2*t^6. + t^6.341 + t^6.373 + 2*t^6.616 + 2*t^6.649 + 4*t^6.681 + t^6.714 + t^6.924 + t^6.957 + 2*t^6.989 + 2*t^7.022 + 2*t^7.054 - t^7.297 - t^7.33 + 3*t^7.362 + 3*t^7.67 + 2*t^7.703 + t^7.913 + t^7.946 + 6*t^7.978 + 2*t^8.011 + 2*t^8.043 + 3*t^8.286 + t^8.319 - 2*t^8.351 + 2*t^8.384 + t^8.594 - t^8.627 - 4*t^8.659 - t^8.692 + 3*t^8.725 + t^8.902 - 2*t^8.967 - t^4.33/y - t^6.681/y - t^6.989/y - t^7.297/y + t^7.362/y + t^7.67/y + t^7.978/y + (2*t^8.011)/y + (2*t^8.319)/y + t^8.351/y + (2*t^8.627)/y + (2*t^8.659)/y + t^8.967/y - t^4.33*y - t^6.681*y - t^6.989*y - t^7.297*y + t^7.362*y + t^7.67*y + t^7.978*y + 2*t^8.011*y + 2*t^8.319*y + t^8.351*y + 2*t^8.627*y + 2*t^8.659*y + t^8.967*y | g1^10*t^2.351 + (2*t^2.659)/g1^4 + t^2.967/g1^18 + t^3. + g1^8*t^3.681 + t^3.957/g1^24 + t^3.989/g1^6 + 2*g1^12*t^4.022 + t^4.33/g1^2 + g1^16*t^4.362 + 2*g1^20*t^4.703 + 2*g1^6*t^5.011 + (4*t^5.319)/g1^8 + g1^10*t^5.351 + t^5.627/g1^22 + t^5.659/g1^4 + t^5.935/g1^36 - 2*t^6. + g1^4*t^6.341 + g1^22*t^6.373 + (2*t^6.616)/g1^28 + (2*t^6.649)/g1^10 + 4*g1^8*t^6.681 + g1^26*t^6.714 + t^6.924/g1^42 + t^6.957/g1^24 + (2*t^6.989)/g1^6 + 2*g1^12*t^7.022 + 2*g1^30*t^7.054 - t^7.297/g1^20 - t^7.33/g1^2 + 3*g1^16*t^7.362 + 3*g1^2*t^7.67 + 2*g1^20*t^7.703 + t^7.913/g1^48 + t^7.946/g1^30 + (6*t^7.978)/g1^12 + 2*g1^6*t^8.011 + 2*g1^24*t^8.043 + (3*t^8.286)/g1^26 + t^8.319/g1^8 - 2*g1^10*t^8.351 + 2*g1^28*t^8.384 + t^8.594/g1^40 - t^8.627/g1^22 - (4*t^8.659)/g1^4 - g1^14*t^8.692 + 3*g1^32*t^8.725 + t^8.902/g1^54 - (2*t^8.967)/g1^18 - t^4.33/(g1^2*y) - (g1^8*t^6.681)/y - t^6.989/(g1^6*y) - t^7.297/(g1^20*y) + (g1^16*t^7.362)/y + (g1^2*t^7.67)/y + t^7.978/(g1^12*y) + (2*g1^6*t^8.011)/y + (2*t^8.319)/(g1^8*y) + (g1^10*t^8.351)/y + (2*t^8.627)/(g1^22*y) + (2*t^8.659)/(g1^4*y) + t^8.967/(g1^18*y) - (t^4.33*y)/g1^2 - g1^8*t^6.681*y - (t^6.989*y)/g1^6 - (t^7.297*y)/g1^20 + g1^16*t^7.362*y + g1^2*t^7.67*y + (t^7.978*y)/g1^12 + 2*g1^6*t^8.011*y + (2*t^8.319*y)/g1^8 + g1^10*t^8.351*y + (2*t^8.627*y)/g1^22 + (2*t^8.659*y)/g1^4 + (t^8.967*y)/g1^18 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 46626 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{1}M_{5}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}$ | 0.6977 | 0.8713 | 0.8008 | [M:[1.1105, 0.7877, 0.6686, 0.9913, 0.8895], q:[0.4346, 0.4549], qb:[0.7776, 0.5538], phi:[0.4448]] | t^2.006 + t^2.363 + 2*t^2.669 + t^2.965 + t^2.974 + t^3.698 + t^3.942 + t^4.003 + t^4.012 + t^4.064 + t^4.3 + t^4.36 + t^4.369 + t^4.657 + 2*t^4.674 + t^4.726 + t^4.971 + t^4.98 + 2*t^5.032 + t^5.329 + 4*t^5.337 + 2*t^5.634 + t^5.643 + t^5.931 + 2*t^5.948 - 3*t^6. - t^4.334/y - t^4.334*y | detail |