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 |
|---|---|---|---|---|---|---|---|---|---|
| 56977 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{7}q_{2}\tilde{q}_{1}$ + ${ }M_{6}M_{7}$ | 0.5757 | 0.7182 | 0.8016 | [M:[1.2798, 0.8254, 0.7202, 0.8809, 1.1468, 1.0139, 0.9861], q:[0.4405, 0.2798], qb:[0.7341, 0.8393], phi:[0.4266]] | [M:[[3], [16], [-3], [-12], [-2], [-7], [7]], q:[[-6], [3]], qb:[[-10], [9]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{3}$, ${ }M_{2}$, ${ }M_{4}$, ${ }M_{7}$, ${ }M_{6}$, ${ }M_{5}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}M_{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{7}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}M_{6}$, ${ }M_{4}^{2}$, ${ }M_{2}M_{7}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{7}$, ${ }M_{4}M_{6}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{7}^{2}$ | ${}$ | -1 | t^2.161 + t^2.476 + t^2.643 + t^2.958 + t^3.042 + 2*t^3.44 + t^3.839 + t^3.923 + t^4.321 + t^4.637 + t^4.72 + t^4.803 + t^4.953 + 2*t^5.119 + t^5.202 + t^5.286 + t^5.435 + 2*t^5.601 + t^5.684 + 2*t^5.917 - t^6. + 3*t^6.083 + t^6.316 + t^6.399 + 2*t^6.482 + t^6.565 + 2*t^6.881 + t^6.964 + t^7.113 + t^7.28 + 2*t^7.363 + t^7.429 + t^7.446 + 2*t^7.595 + 3*t^7.762 + 2*t^7.845 + t^7.911 + t^7.928 + t^8.077 - t^8.161 + 2*t^8.244 + t^8.327 + 2*t^8.393 - 2*t^8.476 + 2*t^8.56 - t^8.643 + 3*t^8.726 + t^8.792 + t^8.875 - 2*t^8.958 - t^4.28/y - t^6.756/y - t^6.923/y + (2*t^7.637)/y + (2*t^7.803)/y + (2*t^8.119)/y + t^8.202/y + t^8.435/y + t^8.518/y + (3*t^8.601)/y + t^8.684/y + (2*t^8.917)/y - t^4.28*y - t^6.756*y - t^6.923*y + 2*t^7.637*y + 2*t^7.803*y + 2*t^8.119*y + t^8.202*y + t^8.435*y + t^8.518*y + 3*t^8.601*y + t^8.684*y + 2*t^8.917*y | t^2.161/g1^3 + g1^16*t^2.476 + t^2.643/g1^12 + g1^7*t^2.958 + t^3.042/g1^7 + (2*t^3.44)/g1^2 + g1^3*t^3.839 + t^3.923/g1^11 + t^4.321/g1^6 + g1^13*t^4.637 + t^4.72/g1 + t^4.803/g1^15 + g1^32*t^4.953 + 2*g1^4*t^5.119 + t^5.202/g1^10 + t^5.286/g1^24 + g1^23*t^5.435 + (2*t^5.601)/g1^5 + t^5.684/g1^19 + 2*g1^14*t^5.917 - t^6. + (3*t^6.083)/g1^14 + g1^19*t^6.316 + g1^5*t^6.399 + (2*t^6.482)/g1^9 + t^6.565/g1^23 + (2*t^6.881)/g1^4 + t^6.964/g1^18 + g1^29*t^7.113 + g1*t^7.28 + (2*t^7.363)/g1^13 + g1^48*t^7.429 + t^7.446/g1^27 + 2*g1^20*t^7.595 + (3*t^7.762)/g1^8 + (2*t^7.845)/g1^22 + g1^39*t^7.911 + t^7.928/g1^36 + g1^11*t^8.077 - t^8.161/g1^3 + (2*t^8.244)/g1^17 + t^8.327/g1^31 + 2*g1^30*t^8.393 - 2*g1^16*t^8.476 + 2*g1^2*t^8.56 - t^8.643/g1^12 + (3*t^8.726)/g1^26 + g1^35*t^8.792 + g1^21*t^8.875 - 2*g1^7*t^8.958 - (g1*t^4.28)/y - (g1^17*t^6.756)/y - t^6.923/(g1^11*y) + (2*g1^13*t^7.637)/y + (2*t^7.803)/(g1^15*y) + (2*g1^4*t^8.119)/y + t^8.202/(g1^10*y) + (g1^23*t^8.435)/y + (g1^9*t^8.518)/y + (3*t^8.601)/(g1^5*y) + t^8.684/(g1^19*y) + (2*g1^14*t^8.917)/y - g1*t^4.28*y - g1^17*t^6.756*y - (t^6.923*y)/g1^11 + 2*g1^13*t^7.637*y + (2*t^7.803*y)/g1^15 + 2*g1^4*t^8.119*y + (t^8.202*y)/g1^10 + g1^23*t^8.435*y + g1^9*t^8.518*y + (3*t^8.601*y)/g1^5 + (t^8.684*y)/g1^19 + 2*g1^14*t^8.917*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 |
|---|---|---|---|---|---|---|---|---|---|
| 55365 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{7}q_{2}\tilde{q}_{1}$ | 0.6596 | 0.8332 | 0.7916 | [M:[1.1456, 0.7427, 0.8544, 0.7847, 1.2363, 0.6939, 0.673], q:[0.3923, 0.4621], qb:[0.8649, 0.7532], phi:[0.3819]] | t^2.019 + t^2.082 + t^2.228 + t^2.354 + t^2.563 + t^3.437 + t^3.5 + 2*t^3.709 + t^4.038 + t^4.101 + t^4.164 + t^4.247 + t^4.31 + t^4.373 + t^4.436 + t^4.456 + 2*t^4.582 + t^4.645 + t^4.708 + t^4.792 + t^4.854 + t^4.917 + t^5.127 + t^5.456 + 2*t^5.518 + t^5.581 + t^5.665 + 2*t^5.728 + 2*t^5.791 + t^5.854 + t^5.937 - 2*t^6. - t^4.146/y - t^4.146*y | detail |