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 |
|---|---|---|---|---|---|---|---|---|---|
| 58491 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }M_{1}M_{2}$ | 1.4531 | 1.6409 | 0.8856 | [X:[1.3328], M:[0.9991, 1.0009], q:[0.497, 0.5022], qb:[0.5004, 0.4987], phi:[0.3336]] | [X:[[0, 2]], M:[[0, 3], [0, -3]], q:[[-1, 15], [-1, -3]], qb:[[1, -6], [1, 0]], phi:[[0, -1]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}^{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$ | ${}$ | -3 | 2*t^2.99 + 2*t^3. + t^3.01 + 2*t^3.99 + 2*t^4. + t^4.01 + 2*t^4.99 + t^5. + t^5.01 + 2*t^5.49 + 2*t^5.5 + t^5.97 + t^5.98 + 4*t^5.99 - 3*t^6. + 4*t^6.01 + t^6.49 + 2*t^6.5 + t^6.51 + t^6.97 + 2*t^6.98 + 5*t^6.99 + 5*t^7. + 5*t^7.01 + t^7.48 + t^7.49 + t^7.51 + t^7.52 + 5*t^7.98 + 5*t^7.99 + 7*t^8. + 6*t^8.01 + t^8.02 + 2*t^8.48 + 2*t^8.49 + t^8.5 - t^8.52 + t^8.96 + t^8.97 + 7*t^8.98 - 2*t^8.99 - t^4./y - t^5./y - (2*t^6.99)/y - (2*t^7.)/y - t^7.01/y - (2*t^7.99)/y - (2*t^8.)/y - t^8.01/y + t^8.98/y + (3*t^8.99)/y - t^4.*y - t^5.*y - 2*t^6.99*y - 2*t^7.*y - t^7.01*y - 2*t^7.99*y - 2*t^8.*y - t^8.01*y + t^8.98*y + 3*t^8.99*y | g2^9*t^2.99 + g2^15*t^2.99 + (2*t^3.)/g2^3 + t^3.01/g2^9 + g2^8*t^3.99 + g2^14*t^3.99 + t^4./g2^4 + g2^2*t^4. + t^4.01/g2^10 + g2^7*t^4.99 + g2^13*t^4.99 + t^5./g2^5 + t^5.01/g2^11 + (g1^3*t^5.49)/g2^7 + (g2^26*t^5.49)/g1^3 + (g1^3*t^5.5)/g2^13 + (g2^8*t^5.5)/g1^3 + g2^30*t^5.97 + g2^24*t^5.98 + 2*g2^6*t^5.99 + 2*g2^12*t^5.99 - 3*t^6. + (2*t^6.01)/g2^12 + (2*t^6.01)/g2^6 + (g2^25*t^6.49)/g1^3 + (g1^3*t^6.5)/g2^14 + (g1^3*t^6.5)/g2^8 + (g2^7*t^6.51)/g1^3 + g2^29*t^6.97 + 2*g2^23*t^6.98 + 4*g2^11*t^6.99 + g2^17*t^6.99 + t^7./g2 + 4*g2^5*t^7. + (3*t^7.01)/g2^13 + (2*t^7.01)/g2^7 + (g2^42*t^7.48)/g1^3 + (g2^24*t^7.49)/g1^3 + (g1^3*t^7.5)/g2^15 + (g1^3*t^7.5)/g2^9 - (g2^12*t^7.5)/g1^3 - (g2^18*t^7.5)/g1^3 + (g2^6*t^7.51)/g1^3 + t^7.52/(g1^3*g2^12) + 3*g2^22*t^7.98 + 2*g2^28*t^7.98 + 4*g2^10*t^7.99 + g2^16*t^7.99 + t^8./g2^2 + 6*g2^4*t^8. + (4*t^8.01)/g2^14 + (2*t^8.01)/g2^8 + t^8.02/g2^20 + g1^3*g2^8*t^8.48 + (g2^41*t^8.48)/g1^3 - (g1^3*t^8.49)/g2^4 + g1^3*g2^2*t^8.49 + (3*g2^23*t^8.49)/g1^3 - (g2^29*t^8.49)/g1^3 + (2*g1^3*t^8.5)/g2^16 + (g1^3*t^8.5)/g2^10 - (2*g2^11*t^8.5)/g1^3 - (g1^3*t^8.51)/g2^28 - (g1^3*t^8.51)/g2^22 + (2*g2^5*t^8.51)/g1^3 - t^8.52/(g1^3*g2^7) + g2^45*t^8.96 + g2^39*t^8.97 + 4*g2^21*t^8.98 + 3*g2^27*t^8.98 + g2^9*t^8.99 - 3*g2^15*t^8.99 - t^4./(g2*y) - t^5./(g2^2*y) - (g2^8*t^6.99)/y - (g2^14*t^6.99)/y - (2*t^7.)/(g2^4*y) - t^7.01/(g2^10*y) - (g2^7*t^7.99)/y - (g2^13*t^7.99)/y - (2*t^8.)/(g2^5*y) - t^8.01/(g2^11*y) + (g2^24*t^8.98)/y + (2*g2^6*t^8.99)/y + (g2^12*t^8.99)/y - (t^4.*y)/g2 - (t^5.*y)/g2^2 - g2^8*t^6.99*y - g2^14*t^6.99*y - (2*t^7.*y)/g2^4 - (t^7.01*y)/g2^10 - g2^7*t^7.99*y - g2^13*t^7.99*y - (2*t^8.*y)/g2^5 - (t^8.01*y)/g2^11 + g2^24*t^8.98*y + 2*g2^6*t^8.99*y + g2^12*t^8.99*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 |
|---|---|---|---|---|---|---|---|---|---|
| 57384 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}^{3}$ | 1.4533 | 1.6416 | 0.8853 | [X:[1.3316], M:[0.9974], q:[0.4909, 0.5065], qb:[0.5013, 0.4961], phi:[0.3342]] | t^2.961 + t^2.977 + t^2.992 + t^3.008 + t^3.023 + t^3.964 + t^3.979 + t^3.995 + t^4.01 + t^4.026 + t^4.966 + t^4.982 + t^5.013 + t^5.029 + t^5.468 + t^5.483 + t^5.498 + t^5.515 + t^5.922 + t^5.938 + t^5.953 + 2*t^5.969 + 2*t^5.984 - 2*t^6. - t^4.003/y - t^5.005/y - t^4.003*y - t^5.005*y | detail |