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 |
|---|---|---|---|---|---|---|---|---|---|
| 2248 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{2}M_{7}$ | 0.6474 | 0.8091 | 0.8001 | [M:[1.1909, 0.7789, 0.8091, 0.8091, 0.8241, 0.7638, 1.2211], q:[0.8015, 0.4196], qb:[0.3894, 0.8015], phi:[0.397]] | [M:[[-6], [-14], [6], [6], [16], [-24], [14]], q:[[1], [13]], qb:[[-7], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{4}$, ${ }M_{5}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{7}$, ${ }q_{1}q_{2}$, ${ }M_{6}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{6}q_{1}q_{2}$ | ${}\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$ | 0 | t^2.291 + t^2.382 + 2*t^2.427 + t^2.472 + t^3.573 + t^3.618 + 2*t^3.663 + t^4.583 + t^4.673 + 2*t^4.718 + 2*t^4.764 + 3*t^4.809 + 4*t^4.854 + 2*t^4.9 + t^4.945 + t^5.864 + t^5.955 + 3*t^6.045 + 4*t^6.091 + 2*t^6.136 + t^6.874 + t^6.965 + 2*t^7.01 + 2*t^7.055 + 2*t^7.1 + 3*t^7.146 + 2*t^7.191 + 5*t^7.236 + 6*t^7.282 + 6*t^7.327 + 2*t^7.372 + t^7.417 + t^8.155 + t^8.246 - t^8.291 - t^8.337 - t^8.382 - t^8.427 + 2*t^8.472 + 6*t^8.518 + 4*t^8.563 + 2*t^8.608 - t^4.191/y - t^6.482/y - t^6.573/y - t^6.618/y - t^6.663/y + t^7.673/y + (3*t^7.718)/y + (2*t^7.764)/y + (3*t^7.809)/y + (2*t^7.854)/y + (3*t^7.9)/y - t^8.774/y + t^8.955/y - t^4.191*y - t^6.482*y - t^6.573*y - t^6.618*y - t^6.663*y + t^7.673*y + 3*t^7.718*y + 2*t^7.764*y + 3*t^7.809*y + 2*t^7.854*y + 3*t^7.9*y - t^8.774*y + t^8.955*y | t^2.291/g1^24 + t^2.382/g1^4 + 2*g1^6*t^2.427 + g1^16*t^2.472 + t^3.573/g1^6 + g1^4*t^3.618 + 2*g1^14*t^3.663 + t^4.583/g1^48 + t^4.673/g1^28 + (2*t^4.718)/g1^18 + (2*t^4.764)/g1^8 + 3*g1^2*t^4.809 + 4*g1^12*t^4.854 + 2*g1^22*t^4.9 + g1^32*t^4.945 + t^5.864/g1^30 + t^5.955/g1^10 + 3*g1^10*t^6.045 + 4*g1^20*t^6.091 + 2*g1^30*t^6.136 + t^6.874/g1^72 + t^6.965/g1^52 + (2*t^7.01)/g1^42 + (2*t^7.055)/g1^32 + (2*t^7.1)/g1^22 + (3*t^7.146)/g1^12 + (2*t^7.191)/g1^2 + 5*g1^8*t^7.236 + 6*g1^18*t^7.282 + 6*g1^28*t^7.327 + 2*g1^38*t^7.372 + g1^48*t^7.417 + t^8.155/g1^54 + t^8.246/g1^34 - t^8.291/g1^24 - t^8.337/g1^14 - t^8.382/g1^4 - g1^6*t^8.427 + 2*g1^16*t^8.472 + 6*g1^26*t^8.518 + 4*g1^36*t^8.563 + 2*g1^46*t^8.608 - t^4.191/(g1^2*y) - t^6.482/(g1^26*y) - t^6.573/(g1^6*y) - (g1^4*t^6.618)/y - (g1^14*t^6.663)/y + t^7.673/(g1^28*y) + (3*t^7.718)/(g1^18*y) + (2*t^7.764)/(g1^8*y) + (3*g1^2*t^7.809)/y + (2*g1^12*t^7.854)/y + (3*g1^22*t^7.9)/y - t^8.774/(g1^50*y) + t^8.955/(g1^10*y) - (t^4.191*y)/g1^2 - (t^6.482*y)/g1^26 - (t^6.573*y)/g1^6 - g1^4*t^6.618*y - g1^14*t^6.663*y + (t^7.673*y)/g1^28 + (3*t^7.718*y)/g1^18 + (2*t^7.764*y)/g1^8 + 3*g1^2*t^7.809*y + 2*g1^12*t^7.854*y + 3*g1^22*t^7.9*y - (t^8.774*y)/g1^50 + (t^8.955*y)/g1^10 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 1211 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ | 0.6654 | 0.8413 | 0.7909 | [M:[1.1857, 0.7667, 0.8143, 0.8143, 0.8381, 0.7428], q:[0.8024, 0.431], qb:[0.3833, 0.8024], phi:[0.3952]] | t^2.229 + t^2.3 + t^2.371 + 2*t^2.443 + t^2.514 + t^3.557 + t^3.629 + t^3.7 + t^4.457 + t^4.528 + 2*t^4.6 + 3*t^4.671 + 4*t^4.743 + 4*t^4.814 + 4*t^4.886 + 2*t^4.957 + t^5.029 + t^5.786 + t^5.857 + t^5.929 + t^6. - t^4.186/y - t^4.186*y | detail |