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 |
|---|---|---|---|---|---|---|---|---|---|
| 1438 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }M_{1}^{2}$ + ${ }M_{3}M_{6}$ | 0.6933 | 0.8493 | 0.8163 | [M:[1.0, 0.984, 1.016, 0.968, 1.032, 0.984], q:[0.508, 0.492], qb:[0.476, 0.54], phi:[0.496]] | [M:[[0], [-4], [4], [-8], [8], [-4]], q:[[2], [-2]], qb:[[-6], [10]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{2}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{5}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}M_{6}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{2}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{1}M_{6}$, ${ }\phi_{1}^{4}$, ${ }M_{1}\phi_{1}^{2}$ | ${}$ | -2 | t^2.904 + 2*t^2.952 + t^2.976 + t^3. + t^3.096 + t^3.144 + t^4.344 + t^4.392 + 2*t^4.44 + t^4.488 + 2*t^4.536 + t^4.584 + t^4.632 + t^4.728 + t^5.856 + t^5.88 + 2*t^5.904 + 2*t^5.928 + t^5.952 + t^5.976 - 2*t^6. + t^6.072 + t^6.096 + t^6.12 + t^6.24 + t^6.288 + t^7.248 + 2*t^7.296 + t^7.32 + 3*t^7.344 + 3*t^7.392 + t^7.416 + 3*t^7.44 - t^7.464 + 3*t^7.488 + t^7.512 + 3*t^7.536 - t^7.56 + 2*t^7.584 + 2*t^7.632 - t^7.656 + 3*t^7.68 + t^7.704 + 2*t^7.728 - t^7.752 + t^7.776 + t^7.824 + t^7.872 + t^8.688 + t^8.736 + 2*t^8.784 + 3*t^8.832 + t^8.856 + 6*t^8.88 - 2*t^8.904 + 4*t^8.928 - 6*t^8.952 + 2*t^8.976 - t^4.488/y - t^7.44/y - t^7.464/y + t^7.512/y + t^7.536/y + (2*t^8.856)/y + t^8.88/y + (2*t^8.904)/y + (2*t^8.928)/y + (2*t^8.952)/y + t^8.976/y - t^4.488*y - t^7.44*y - t^7.464*y + t^7.512*y + t^7.536*y + 2*t^8.856*y + t^8.88*y + 2*t^8.904*y + 2*t^8.928*y + 2*t^8.952*y + t^8.976*y | t^2.904/g1^8 + (2*t^2.952)/g1^4 + t^2.976/g1^2 + t^3. + g1^8*t^3.096 + g1^12*t^3.144 + t^4.344/g1^13 + t^4.392/g1^9 + (2*t^4.44)/g1^5 + t^4.488/g1 + 2*g1^3*t^4.536 + g1^7*t^4.584 + g1^11*t^4.632 + g1^19*t^4.728 + t^5.856/g1^12 + t^5.88/g1^10 + (2*t^5.904)/g1^8 + (2*t^5.928)/g1^6 + t^5.952/g1^4 + t^5.976/g1^2 - 2*t^6. + g1^6*t^6.072 + g1^8*t^6.096 + g1^10*t^6.12 + g1^20*t^6.24 + g1^24*t^6.288 + t^7.248/g1^21 + (2*t^7.296)/g1^17 + t^7.32/g1^15 + (3*t^7.344)/g1^13 + (3*t^7.392)/g1^9 + t^7.416/g1^7 + (3*t^7.44)/g1^5 - t^7.464/g1^3 + (3*t^7.488)/g1 + g1*t^7.512 + 3*g1^3*t^7.536 - g1^5*t^7.56 + 2*g1^7*t^7.584 + 2*g1^11*t^7.632 - g1^13*t^7.656 + 3*g1^15*t^7.68 + g1^17*t^7.704 + 2*g1^19*t^7.728 - g1^21*t^7.752 + g1^23*t^7.776 + g1^27*t^7.824 + g1^31*t^7.872 + t^8.688/g1^26 + t^8.736/g1^22 + (2*t^8.784)/g1^18 + (3*t^8.832)/g1^14 + t^8.856/g1^12 + (6*t^8.88)/g1^10 - (2*t^8.904)/g1^8 + (4*t^8.928)/g1^6 - (6*t^8.952)/g1^4 + (2*t^8.976)/g1^2 - t^4.488/(g1*y) - t^7.44/(g1^5*y) - t^7.464/(g1^3*y) + (g1*t^7.512)/y + (g1^3*t^7.536)/y + (2*t^8.856)/(g1^12*y) + t^8.88/(g1^10*y) + (2*t^8.904)/(g1^8*y) + (2*t^8.928)/(g1^6*y) + (2*t^8.952)/(g1^4*y) + t^8.976/(g1^2*y) - (t^4.488*y)/g1 - (t^7.44*y)/g1^5 - (t^7.464*y)/g1^3 + g1*t^7.512*y + g1^3*t^7.536*y + (2*t^8.856*y)/g1^12 + (t^8.88*y)/g1^10 + (2*t^8.904*y)/g1^8 + (2*t^8.928*y)/g1^6 + (2*t^8.952*y)/g1^4 + (t^8.976*y)/g1^2 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 937 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }M_{1}^{2}$ | 0.6921 | 0.8476 | 0.8165 | [M:[1.0, 0.9903, 1.0097, 0.9807, 1.0193], q:[0.5048, 0.4952], qb:[0.4855, 0.5242], phi:[0.4976]] | t^2.942 + t^2.971 + t^2.985 + t^3. + t^3.029 + t^3.058 + t^3.087 + t^4.406 + t^4.435 + 2*t^4.464 + t^4.493 + 2*t^4.522 + t^4.551 + t^4.58 + t^4.638 + t^5.927 + t^5.956 + t^5.971 + t^5.985 - t^6. - t^4.493/y - t^4.493*y | detail |